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  <front>
    <journal-meta><journal-id journal-id-type="publisher">HESS</journal-id><journal-title-group>
    <journal-title>Hydrology and Earth System Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">HESS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Hydrol. Earth Syst. Sci.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1607-7938</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/hess-22-6087-2018</article-id><title-group><article-title>Understanding the water cycle over the upper Tarim Basin: retrospecting the estimated discharge bias to atmospheric<?xmltex \hack{\break}?>
variables and model structure</article-title><alt-title>Retrospecting the estimated discharge bias</alt-title>
      </title-group><?xmltex \runningtitle{Retrospecting the estimated discharge bias}?><?xmltex \runningauthor{X. Zhou et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Zhou</surname><given-names>Xudong</given-names></name>
          <email>xudong.zhou@lmd.polytechnique.fr</email>
        <ext-link>https://orcid.org/0000-0001-7180-8187</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Polcher</surname><given-names>Jan</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-9020-5795</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Yang</surname><given-names>Tao</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2502-0353</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Hirabayashi</surname><given-names>Yukiko</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5693-197X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Nguyen-Quang</surname><given-names>Trung</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8776-2635</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>State Key Laboratory of Hydrology-Water Resources and Hydraulic Engineering, Hohai University, <?xmltex \hack{\break}?>210098, Nanjing, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Laboratoire de Météorologie Dynamique du CNRS, IPSL, École Polytechnique, 91128, Paris, France</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Civil Engineering, Shibaura Institute of Technology, Tokyo, Japan</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Xudong Zhou (xudong.zhou@lmd.polytechnique.fr)</corresp></author-notes><pub-date><day>28</day><month>November</month><year>2018</year></pub-date>
      
      <volume>22</volume>
      <issue>11</issue>
      <fpage>6087</fpage><lpage>6108</lpage>
      <history>
        <date date-type="received"><day>22</day><month>February</month><year>2018</year></date>
           <date date-type="rev-request"><day>28</day><month>March</month><year>2018</year></date>
           <date date-type="rev-recd"><day>18</day><month>July</month><year>2018</year></date>
           <date date-type="accepted"><day>1</day><month>November</month><year>2018</year></date>
      </history>
      <permissions>
        
        
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018.html">This article is available from https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018.html</self-uri><self-uri xlink:href="https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018.pdf">The full text article is available as a PDF file from https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018.pdf</self-uri>
      <abstract>
    <p id="d1e134">The bias in atmospheric variables and that in model computation are
two major causes of failures in discharge estimation. Attributing the bias in
discharge estimation becomes difficult if the forcing bias cannot be
evaluated and excluded in advance in places lacking qualified meteorological
observations, especially in cold and mountainous areas (e.g., the upper
Tarim Basin). In this study, we proposed an Organizing Carbon and Hydrology In Dynamic
EcosystEms (ORCHIDEE)-Budyko framework which
helps identify the bias range from the two sources (i.e., forcing and model
structure) with a set of analytical approaches. The latest version of the land
surface model ORCHIDEE was used to provide reliable discharge simulations
based on the most improved forcing inputs. The Budyko approach was then
introduced to attribute the discharge bias to two sources with prescribed
assumptions. Results show that, as the forcing biases, the water inputs
(rainfall, snowfall or glacier melt) are very likely underestimated for the
Tarim headwater catchments (<inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">43.2</mml:mn></mml:mrow></mml:math></inline-formula> % to 21.0 %). Meanwhile, the
potential evapotranspiration is unrealistically high over the upper Yarkand
and the upper Hotan River (1240.4 and 1153.7 mm yr<inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively). Determined by the model structure, the bias in actual
evapotranspiration is possible but not the only contributor to the discharge
underestimation (overestimated by up to 105.8 % for the upper Aksu River). Based
on a simple scaling approach, we estimated the water consumption by human
intervention ranging from <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mn mathvariant="normal">213.50</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>  to
<inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mn mathvariant="normal">300.58</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> at the Alar gauge station, which is
another bias source in the current version of ORCHIDEE. This study succeeded
in retrospecting the bias from the discharge estimation to multiple bias
sources of the atmospheric variables and the model structure. The framework
provides a unique method for evaluating the regional water cycle and its
biases with our current knowledge of observational uncertainties.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e218">A failure of discharge estimation can easily happen to a researcher
especially when exploring a new region. It is often attributed to model
inapplicability to the region, and tuning the model parameters is a common
way to eliminate the discharge bias <xref ref-type="bibr" rid="bib1.bibx58 bib1.bibx80" id="paren.1"/>.
However, a hidden assumption is often ignored that the atmospheric variables
(or named here forcing) are essentially correct, while it may fail in some
regions <xref ref-type="bibr" rid="bib1.bibx25 bib1.bibx1" id="paren.2"/>. Without knowing the bias in forcing,
the calibration becomes meaningless if the model parameters are tuned to
values that are far from their physical meaning <xref ref-type="bibr" rid="bib1.bibx35 bib1.bibx56 bib1.bibx57" id="paren.3"/>. Thus, an important step before applying a model to a new
region is to understand where the bias sources lie and their relative
relations <xref ref-type="bibr" rid="bib1.bibx60" id="paren.4"/>.</p>
      <p id="d1e233">In situ measurements are considered most reliable sources for
atmospheric variables and thus can be used to evaluate or further correct the
variables used to drive hydrological models <xref ref-type="bibr" rid="bib1.bibx73" id="paren.5"/>. However,
larger uncertainties are still<?pagebreak page6088?> found in mountainous and arid areas due to the
poor representativity of in situ observations <xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx34 bib1.bibx86 bib1.bibx74" id="paren.6"/>. For instance, the precipitation (<inline-formula><mml:math id="M7" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) over the
mountainous area is mostly underestimated due to rare observations at high
altitude and orographic effects <xref ref-type="bibr" rid="bib1.bibx34" id="paren.7"/>. A total of 20.2 % of the
precipitation is underestimated over global orographically affected regions
according to <xref ref-type="bibr" rid="bib1.bibx1" id="text.8"/>. Arid areas receive less water input but have
larger relative uncertainties in precipitation <xref ref-type="bibr" rid="bib1.bibx25" id="paren.9"/>, which are
crucial to regional runoff (<inline-formula><mml:math id="M8" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>) generation. Meanwhile, the energy flux over arid
regions varies significantly. Thus the potential evapotranspiration (PET)
and the actual evapotranspiration (ET) are quite uncertain over those
areas <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx79" id="paren.10"/>; in the meanwhile, the PET and ET are
variables unable to directly measure for a basin. Investigation of their
errors and relations based on the model simulation becomes necessary.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><caption><p id="d1e271">The major rivers and the glacier distribution in the Tarim Basin.
The upper Yarkand River catchment is defined by hydrological gauges 1 (JK) and 2
(KQ), the upper Hotan River catchment is defined by hydrological gauges 3 (TGZLK) and
4 (WLWT), and the upper Aksu River catchment is defined by hydrological gauges 5
(SLGLK) and 6 (XHL). The upper Tarim Basin is defined by hydrological gauge 7 (Alar).</p></caption>
        <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018-f01.pdf"/>

      </fig>

      <p id="d1e280">Model efficiency needs to be verified firstly. The model performance is
generally evaluated on the agreement of a single variable, and discharge is
the most commonly used as it is the result of all the water–energy processes.
It reveals the accuracy of the whole system while also accumulating all the
errors from the forcing and the model. Therefore, a multivariable analysis
based on the relation between variables is needed for overall evaluation
<xref ref-type="bibr" rid="bib1.bibx41" id="paren.11"/>. These relations represent typical climatic and regional
characteristics; i.e., the aridity index (PET <inline-formula><mml:math id="M9" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M10" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) reveals the energy and
water input over a specific region <xref ref-type="bibr" rid="bib1.bibx100 bib1.bibx101" id="paren.12"/>, and the
ratio of evapotranspiration to precipitation (ET <inline-formula><mml:math id="M11" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M12" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) is relevant to the land
cover conditions <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx85" id="paren.13"/>. The Budyko hypothesis is a widely
accepted empirical relation between ET <inline-formula><mml:math id="M13" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M14" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> and PET <inline-formula><mml:math id="M15" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M16" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx8" id="paren.14"/>.
The shape of the optimal Budyko curve reflects local climatic and underlying
characteristics <xref ref-type="bibr" rid="bib1.bibx53 bib1.bibx84" id="paren.15"/>. Hence with a Budyko curve
derived from land surface model simulations, biases of the water–energy
components (<inline-formula><mml:math id="M17" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, ET or PET) can be assessed. For example, <xref ref-type="bibr" rid="bib1.bibx1" id="text.16"/>
quantified the precipitation bias in orographically affected areas using the
Budyko hypothesis, although their work attributed all the bias in discharge
simulation to the forcing with an incorrect assumption that their model was
perfect.</p>
      <p id="d1e367">Most of the hydrological models, with either a lumped or a distributed concept,
are dependent on the calibration. Because of the assumption that water input
(<inline-formula><mml:math id="M18" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) is correct and a very crude description of energy processes, the ET is
the variables which can be adjusted to meet the water mass balance. Most of
the bias is therefore assumed to derive from the ET. It may mislead the
relations between PET <inline-formula><mml:math id="M19" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M20" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> and ET <inline-formula><mml:math id="M21" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M22" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, which represents the climatic and
regional characteristics <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx100 bib1.bibx85 bib1.bibx101" id="paren.17"/>.
Land surface models (LSMs) are almost independent of the calibration process,
with most of the model parameters obtained from multiple maps (e.g., land
cover, land use, soil textures). Based on their substantial
physically based modules, the LSMs have been widely used to estimate most of
the components in the continental water cycle <xref ref-type="bibr" rid="bib1.bibx92 bib1.bibx91 bib1.bibx51 bib1.bibx71 bib1.bibx60" id="paren.18"/>. Although the LSMs do not necessarily
provide good estimates of discharge <xref ref-type="bibr" rid="bib1.bibx30 bib1.bibx25 bib1.bibx93 bib1.bibx42" id="paren.19"/>, they prevent all the bias being revised by calibration. In
return, the modeled discharge bias can reveal the biases related to model
input or model structure, which have not attracted enough attention.</p>
      <p id="d1e415">The Tarim Basin – located in the northwest of China, central Asia; surrounded
by high mountains; and punctuated by oases in the center of deserts – is a region integrating
the mountainous, arid and cold characteristics in different parts
<xref ref-type="bibr" rid="bib1.bibx87 bib1.bibx88" id="paren.20"/>. The precipitation is mainly distributed over the
upper mountainous area around the boundaries, and the snowmelt and glacier melt
are major contributors to the local water resources <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx55" id="paren.21"/>. However, the meteorologic observations on the water input
components are sparse, and the gauges are not representative because the
surface conditions are heterogeneous especially in the mountainous area
<xref ref-type="bibr" rid="bib1.bibx64" id="paren.22"/>. In the lower oases, intensive irrigation is developed,
which is hugely reliant on the discharge flowing from the headwater catchments
<xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx59" id="paren.23"/>, causing considerable changes in the natural
river discharge downstream of the area <xref ref-type="bibr" rid="bib1.bibx99 bib1.bibx69" id="paren.24"/>. In
reality, human intervention is very difficult to model as it is policy
related and because of the lack of an efficient dataset. The anthropogenic
effects on the water cycle, accompanying the climatic and topographic
characteristics, make the Tarim one of the most challenging places to apply
land surface models.</p>
      <p id="d1e433">There are three major steps in this study, Firstly, we generated a
best-possible forcing dataset for the Tarim domain which reduces as far as
possible the biases using refined data sets. The refined forcing then drove
an improved land surface model (Organizing Carbon and Hydrology In Dynamic
EcosystEms: ORCHIDEE) to obtain the improved discharge
estimations. Secondly, the estimated discharge was compared with
in situ discharge observations (Sect. 4.1), and the evidence of
their bias analyzed (Sect. 4.2). In the third step, the possible bias
sources from the forcing and model structure were qualified with the Budyko
hypothesis (Sect. 4.3), and their possibilities are discussed in Sect. 4.4. The
model bias due to ignorance of human intervention is estimated based on the
bias analysis over the headwater catchments in Sect. 4.5.</p>
</sec>
<sec id="Ch1.S2">
  <title>Study area and hydrometeorological characteristics</title>
      <?pagebreak page6089?><p id="d1e442">The Tarim Basin locates in the northwest of China, surrounded by the Kunlun
Mountains in the south, the Tienshan Mountain in the north and the Pamirs
Plateau in the west (Fig. <xref ref-type="fig" rid="Ch1.F1"/>). Its U-shaped terrain blocks
the westerly atmospheric water vapor transport that leads to relatively low
precipitation inside the basin <xref ref-type="bibr" rid="bib1.bibx82" id="paren.25"/>. As simulated by <xref ref-type="bibr" rid="bib1.bibx82" id="text.26"/>,
63 % of the water vapor enters Tarim through the eastern passway, but
it only happens in summer, contributing around 54 % of the total annual
precipitation, leading to a strong seasonality in precipitation
<xref ref-type="bibr" rid="bib1.bibx69" id="paren.27"/>. Combined with the glacier melt during warm summer, 70 %
of the annual discharge is concentrated in the period from June to October
<xref ref-type="bibr" rid="bib1.bibx45" id="paren.28"/>. The high seasonality implies a high risk of water deficit
in dry seasons and endangers the ecosystem along the rivers
<xref ref-type="bibr" rid="bib1.bibx19" id="paren.29"/>, which requires human regulation to allow for efficient agriculture.</p>
      <p id="d1e463">Despite the high interannual variability, the precipitation is
heterogeneously distributed due to orographic effects <xref ref-type="bibr" rid="bib1.bibx82" id="paren.30"/>. It
ranges from 200 to 500 mm yr<inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in the mountainous area, while there is less
than 50 mm in the central Tarim <xref ref-type="bibr" rid="bib1.bibx11" id="paren.31"/>. The mountainous
glacier melt/snowmelt occurs in the same place where precipitation is generated.
The mountainous area contributes almost all the river runoff of the Tarim
Basin, while the plains of Tarim contribute little to the water resource of
the main Tarim <xref ref-type="bibr" rid="bib1.bibx88 bib1.bibx65" id="paren.32"/>. In the upper Tarim, only three
water systems (the Yarkand, the Hotan and the Aksu rivers; see Fig. 1) have natural
hydraulic connections to the mainstream – the Tarim <xref ref-type="bibr" rid="bib1.bibx88" id="paren.33"/>. The
water originating from the mountains flows through the oases where people
live and allows intensive agriculture <xref ref-type="bibr" rid="bib1.bibx46" id="paren.34"/>. As a
consequence, a large proportion of the water is extracted for human
utilization in the oases, so that only 8.7 %, 43.4 % and 30.6 %
of the discharge from headwater regions of the Yarkand, Hotan and Aksu rivers can
finally reach Tarim mainstream, respectively <xref ref-type="bibr" rid="bib1.bibx99" id="paren.35"><named-content content-type="pre">25.3 % overall in
1995;</named-content></xref>. The Kaxgar River is another major tributary of the Tarim, but
it has already dried up before water could reach the mainstream due to natural
evaporation/leakage and human intervention. Of all the water consumption,
agriculture irrigation accounts for more than 95 % in the Tarim Basin
<xref ref-type="bibr" rid="bib1.bibx99" id="paren.36"/>; hence the dominant human influence in the Tarim Basin is considered
to be the irrigation influence.</p>
      <p id="d1e502">There are 11 665 glaciers with a total area of 19 878 km<inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> and a
volume of 2313 km<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> distributed over the Tarim <xref ref-type="bibr" rid="bib1.bibx44" id="paren.37"/>. The
glacier melt is a critical contributor to the local water resource. According
to <xref ref-type="bibr" rid="bib1.bibx99" id="text.38"/> and <xref ref-type="bibr" rid="bib1.bibx63" id="text.39"/>, the estimated glacier melt
accounts for around 40 % of the total river runoff for the whole Tarim.
However, due to the climate change, a large number of the glaciers were in
retreat during the last 40 years (1960s–2001). In the upper Tarim, the
Yarkand River has suffered the most significant glacier area changes
(<inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">205</mml:mn></mml:mrow></mml:math></inline-formula> km<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>) with a relative proportion of <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6.1</mml:mn></mml:mrow></mml:math></inline-formula> %. The most
significant retreat rate (<inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">7.9</mml:mn></mml:mrow></mml:math></inline-formula> %) in glacier area occurs on the Pamirs
Plateau in the west <xref ref-type="bibr" rid="bib1.bibx63" id="paren.40"/>. All the changes in glaciers will
result in the alteration in the river discharge and also the human
interactions.</p>
</sec>
<?pagebreak page6090?><sec id="Ch1.S3">
  <title>Data and models</title>
<sec id="Ch1.S3.SS1">
  <title>Data and simulation description</title>
<sec id="Ch1.S3.SS1.SSS1">
  <title>River discharge observations</title>
      <p id="d1e591">River discharge is a very reliable and integrated observation of the
continental water cycle which is always used as a validation variable
<xref ref-type="bibr" rid="bib1.bibx89" id="paren.41"/>. Over the headwater catchments, there are 13 hydrological
gauges recorded in the Hydrological Yearbooks of China
issued by the Ministry of Water Resources, though only six gauges are
selected with consideration of their locations and data completeness. Two
gauges (1, 2) are in the upper Yarkand River, two (3, 4) are in the upper
Hotan River, and two (5, 6) are in the upper Aksu River, while no gauge is
found on the Kaxgar River. For the gauges in headwater catchments, the
discharge is considered free of human intervention, i.e., irrigation or
reservoir regulation, so to a large extent they represent the natural
environment <xref ref-type="bibr" rid="bib1.bibx13" id="paren.42"/>. This facilitates model validation. Moreover, on
the mainstream of Tarim, one gauge (7, Alar) was selected at the junction of
three upstream rivers (Fig. <xref ref-type="fig" rid="Ch1.F1"/>). Different from the
headwater gauges, the river discharge at Alar has been significantly altered
by human consumption after flowing through the irrigation area
<xref ref-type="bibr" rid="bib1.bibx46" id="paren.43"/>. Hence, the observations are no longer natural values
but can be used to quantify the influence resulting from human activities.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS2">
  <title>Near-surface atmospheric conditions</title>
      <p id="d1e611">Near-surface atmospheric conditions are crucial to hydrological responses
<xref ref-type="bibr" rid="bib1.bibx1" id="paren.44"/>. However, both the model simulation and gridded forcing
generated from observations are proven to have large uncertainties where
observations are sparse and heterogeneity is strong <xref ref-type="bibr" rid="bib1.bibx34 bib1.bibx22" id="paren.45"/>, i.e., in the arid and mountainous area, so that, in practice,
several forcing datasets are always used in parallel to generate an ensemble
of climate conditions which hopefully tracks the uncertainties
<xref ref-type="bibr" rid="bib1.bibx42 bib1.bibx70" id="paren.46"/>. Alternatively, when possible, regional
datasets which contain more information than global datasets are used to move
the forcing closer to true values <xref ref-type="bibr" rid="bib1.bibx39" id="paren.47"/>. In this study, several
sets of estimated forcing inputs based on WATCH (Water and Global Change;
<xref ref-type="bibr" rid="bib1.bibx33" id="altparen.48"/>; <xref ref-type="bibr" rid="bib1.bibx77" id="altparen.49"/>) are developed and then used to drive the
land surface model (Fig. <xref ref-type="fig" rid="Ch1.F2"/>). The best simulations among them
will be used to analyze the accompanying bias with its driving forcing.</p>
      <p id="d1e635">A pair of reference forcing datasets are WFD (WATCH Forcing Data, 1958–2001;
<xref ref-type="bibr" rid="bib1.bibx75 bib1.bibx76" id="altparen.50"/>) and WFDEI (WATCH Forcing Data methodology
applied to ERA-Interim data, 1979–2012; <xref ref-type="bibr" rid="bib1.bibx77 bib1.bibx78" id="altparen.51"/>).
They use the same methodologies but have slight differences in the basic
data, processing and formatting <xref ref-type="bibr" rid="bib1.bibx77" id="paren.52"/>. In brief, WFDEI is an
evolution of WFD where the underlying re-analysis is now ERA-Interim but
using the same bias correction methodology. This product has been proven to
be superior to WFD. CRU (Climate Research Unit) monthly total precipitation
observations were used to bias-correct the precipitation in WFD and WFDEI
datasets. However, the WFD uses a previous version CRU TS 2.10 before the CRU
TS 3.1 used in WFDEI was released <xref ref-type="bibr" rid="bib1.bibx77" id="paren.53"/>. The two CRU datasets
differ in the time period (CRU TS 2.10: 1901–2002; CRU TS 3.1: 1979–2009;
<xref ref-type="bibr" rid="bib1.bibx40" id="altparen.54"/>),
in the stations used and in the methods employed; see <xref ref-type="bibr" rid="bib1.bibx34" id="paren.55"/> for
details. Hence, there are still some differences between the two which could
further affect the hydrological responses. The two datasets are named WFD-CRU
and WFDEI-CRU for later description, and the time step for all the forcing
variables is 3 h.</p>
      <p id="d1e657">The CRU datasets were constructed by monthly observations at meteorological
stations across the world's continents. The observations were then
interpolated to 0.5<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> longitude–latitude grid cells. Though the CRU
compares favorably to some other gridded datasets, it has significant
deviations over regions and time periods with sparser observational data
<xref ref-type="bibr" rid="bib1.bibx34" id="paren.56"/>. Moreover, because only the monthly total precipitation
was used to correct WFDEI and WFD, it cannot improve the temporal
variabilities at smaller time steps (i.e., daily or sub-daily). However, the
precipitation variations in a short period would result in different
hydrological responses even in the condition of the total monthly amount
remaining the same <xref ref-type="bibr" rid="bib1.bibx54" id="paren.57"/>.</p>
      <p id="d1e675">Hence, in addition, the WFDEI-CRU dataset was further corrected by the
gridded daily precipitation data from the China Meteorological Administration
(named CMA). The CMA precipitation product compiles 2416 national
meteorological monitoring stations over China, using the climatological
optimal interpolation method to generate the gridded 0.5<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
precipitation field from 1951 to 2016 (<xref ref-type="bibr" rid="bib1.bibx98 bib1.bibx64" id="altparen.58"/>). PRISM
(Parameter-elevation Regression on Independent Sloped Methods;
<xref ref-type="bibr" rid="bib1.bibx14" id="altparen.59"/>) was used to lessen the orographic effects
<xref ref-type="bibr" rid="bib1.bibx64" id="paren.60"/>. The density of meteorological stations used in the CMA is
much higher than that used for CRU. For instance, there are only six gauges
over the Tarim Basin in the CRU database, while 39 gauges are recorded in the
CMA system <xref ref-type="bibr" rid="bib1.bibx69" id="paren.61"/> so that it can to a certain degree improve the
data applicability where precipitation is spatially inhomogeneous compared to
CRU datasets. Given that the CMA data provide the daily information, it also
improves the temporal variations of precipitation rather than using the total
monthly value in CRU datasets. The corrected atmospheric input dataset is
hereafter referred to as WFDEI-CMA.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS3">
  <title>Glacier melt dataset</title>
      <p id="d1e705">As mentioned in Sect. 2, glacier melt is a vital water input to the Tarim.
However, glacier runoff measurement is so<?pagebreak page6091?> difficult for such large regions
that model-based estimates of the glacier melt are necessary. In general,
a glacier module is not coupled in LSMs <xref ref-type="bibr" rid="bib1.bibx26" id="paren.62"/>. Hence, rather
than building a separate glacier module, we use an independent daily glacier
melt dataset obtained from the glacier model called HYOGA2 (meaning <italic>glacier</italic> in Japanese), which has been
proven reliable over the globe <xref ref-type="bibr" rid="bib1.bibx37" id="paren.63"/>. HYOGA2 is a
temperature-index-based model utilizing an extensive global-scale glacier
inventory and has several improvements compared to its first version (HYOGA) in
model parameter simulation as well as the temporal extent. More details can
be found in the original papers <xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx37" id="paren.64"/>. The
glacier melt is added to the rainfall series of WFDEI-CMA as an additional
water flux to the system. The melt water hence participates
instantaneously in the water cycle without delays such as stores in ice,
glacier pack or groundwater recharge beneath the ice being considered. This
method was chosen for its simplicity and the lack of knowledge on the details
at the transition between the glacier and the soil. Daily values are
uniformly distributed over the eight time steps per day of WFDEI. By adding the
glacier melt, the fourth new forcing dataset is generated as WFDEI-CCG.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS2">
  <title>ORCHIDEE land surface model</title>
      <p id="d1e727">The land surface model ORCHIDEE (Organizing Carbon and Hydrology In Dynamic
EcosystEms) was developed by the Laboratoire de Météorologie
Dynamique (IPSL-LMD) <xref ref-type="bibr" rid="bib1.bibx23 bib1.bibx15 bib1.bibx21" id="paren.65"/>. After
more than 20 years of development, ORCHIDEE has been validated from the
global scale <xref ref-type="bibr" rid="bib1.bibx2" id="paren.66"/> to typical regional cases, e.g., tropical
rainforest area <xref ref-type="bibr" rid="bib1.bibx32" id="paren.67"><named-content content-type="pre">Amazon;</named-content></xref>, semiarid regions
<xref ref-type="bibr" rid="bib1.bibx22" id="paren.68"><named-content content-type="pre">western Africa;</named-content></xref> and middle-latitude regions
<xref ref-type="bibr" rid="bib1.bibx68" id="paren.69"><named-content content-type="pre">Europe;</named-content></xref>. Within ORCHIDEE, only SECHIBA
(Schematisation des Echanges Hydriques I'Interface entre la Biosphere et
I'atmosphere), which represents the energy and water fluxes between land
surfaces and the atmosphere, is used in this study. The hydrological module
in SECHIBA is based on developments by <xref ref-type="bibr" rid="bib1.bibx17" id="text.70"/> and
<xref ref-type="bibr" rid="bib1.bibx20" id="text.71"/>. Thirteen types of vegetation are defined
<xref ref-type="bibr" rid="bib1.bibx21" id="paren.72"/>, and dynamic leaf area index is computed to generate the
interception and transpiration. The vertical soil water movement is
represented by diffusion-type equations resolved on a fine vertical
discretization (11 levels) and partitioning between infiltration and surface
runoff through a time-splitting procedure <xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx21 bib1.bibx32" id="paren.73"/>. The routing is conducted based on a linear reservoir
concept through redefined routing units which are different from the
atmospheric grids <xref ref-type="bibr" rid="bib1.bibx32" id="paren.74"/>. The ORCHIDEE version used in this
study is available at <uri>https://forge.ipsl.jussieu.fr/orchidee/</uri>
(<xref ref-type="bibr" rid="bib1.bibx48" id="altparen.75"/>).</p><?xmltex \hack{\newpage}?>
<sec id="Ch1.S3.SS2.SSS1">
  <title>Evapotranspiration simulation</title>
      <p id="d1e780">On top of precipitation, evapotranspiration and potential evapotranspiration
are two important fluxes, and their errors are key to the water cycle
modeling. In ORCHIDEE, the evapotranspiration is calculated with energy
balance and resistance concepts. The potential evapotranspiration is defined
as “the amount of evapotranspiration that would occur if enough water was
available at the surface”, as explained in <xref ref-type="bibr" rid="bib1.bibx3" id="text.76"/>. The
PET is computed as the sum of the potential soil evaporation and the
potential transpiration from vegetation. For soil evaporation, the diffusive
equations are taken with the ratio of the humidity gradient, the aerodynamic
resistance and the air density. The virtual surface temperature is used
instead of the actual one to compute the saturate humidity, while the virtual
surface temperature is calculated through an unstressed surface energy
balance. The method has been proven superior to other diffusive methods in
the reference paper <xref ref-type="bibr" rid="bib1.bibx3" id="text.77"/>. The potential transpiration is
driven by the potential evaporation between the evaporating surface and the
overlying air but is limited by vegetation resistances. The maximal water loss
under stress-free conditions is the potential transpiration
<xref ref-type="bibr" rid="bib1.bibx32" id="paren.78"/>. The actual evapotranspiration is a function of the
potential evaporation but is modeled by a series of resistances (canopy and
aerodynamics) of the surface layer. The details of the methods in simulating
PET and ET can be found in <xref ref-type="bibr" rid="bib1.bibx20" id="text.79"/>, <xref ref-type="bibr" rid="bib1.bibx32" id="text.80"/>
and <xref ref-type="bibr" rid="bib1.bibx3" id="text.81"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><caption><p id="d1e804">The flowchart of the five experiments designed for driving the ORCHIDEE
in this study. WFD and WFDEI are two basic forcing datasets. The underlined
terms with numbers are the five experiments, while the grey arrows represent the
development of the forcing compared to their previous ones.</p></caption>
            <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018-f02.pdf"/>

          </fig>

</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <title>Snow and soil freezing scheme</title>
      <?pagebreak page6092?><p id="d1e819">There is on key improvement which has been implemented in the current version
of ORCHIDEE, that is, the snow and soil freezing scheme. Snow and soil
freezing are two crucial water processes in cold regions; snow covers nearly
half of land area <xref ref-type="bibr" rid="bib1.bibx72" id="paren.82"/>, and the frozen soils occupy 55 % to
60 % of the land surface of the Northern Hemisphere in winter
<xref ref-type="bibr" rid="bib1.bibx97" id="paren.83"/>. Snow plays an important role in both the energy and water
flux as the snow cover is first an insulation which prevents the heat loss
from the soil. It also increases the thermal inertia of the surface by adding
a new phase change and acts as a moisture reservoir which stores winter
precipitation that is released in spring or early summer. In the old ORCHIDEE
version, a constant density and very simple heat capacity are applied for the
snow. The snowmelt directly feeds the runoff without refreezing, and the snow
layer is mixed with the first soil layer so that they are equal in
temperature. While in the new snow scheme, the snow layer is defined and
separated from the soil layers. The snowpack is represented in three layers
which adequately resolve the snow thermal gradients between the top and base
of the snow cover. The energy balance and the temperature of the snow body
become more realistic. Refreezing of the snowmelt is allowed, which makes the
energy changes more reliable. The snow properties are more detailed than
before, i.e., the density, albedo and roughness. All the improvements have
been validated over France and northern Eurasia and already implemented in
the current ORCHIDEE <xref ref-type="bibr" rid="bib1.bibx72" id="paren.84"/>.</p>
      <p id="d1e831">Soil freezing impedes water infiltration and drainage, thus leading to changes
in hydrological responses <xref ref-type="bibr" rid="bib1.bibx81" id="paren.85"/>. At small scales, the soil freezing
alters the soil structure and therefore its water capacity, which has a
consequence on the water flux between soil and atmosphere, as well as the
water availability for plants <xref ref-type="bibr" rid="bib1.bibx52 bib1.bibx38" id="paren.86"/>. On the other
hand, the frozen soil changes the latent heat exchange, which delays the soil
temperature signal <xref ref-type="bibr" rid="bib1.bibx7" id="paren.87"/>. Soil thermal characteristics are also
improved due to the different thermal properties of ice and water. In the old
soil thermal equations, thermal advection and phase change of the water are
not considered when resolving the latent heat exchanges
<xref ref-type="bibr" rid="bib1.bibx31" id="paren.88"/>. The mechanical effects of soil freezing are therefore
ignored. In the new soil freezing scheme, the apparent soil heat capacity can
be increased by considering the ice content of the soil layer during a
freezing-temperature window between 0 and <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. A temperature
correction is applied if any soil layer is entirely frozen or thawed.
Moreover, the soil heat conductivity is changeable according to the ice
content in the soil, which affects the thermal propagation in the vertical
soil column. Finally, the hydraulic conductivity is reduced as a function of
the ice content. Liquid water is not allowed to cross the frozen soil layers.
Thus infiltration and drainage are forced to stop. Full descriptions of the
new freezing soil equations and the parameterizations setting can be found in
<xref ref-type="bibr" rid="bib1.bibx31" id="text.89"/>.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS3">
  <title>Human intervention</title>
      <p id="d1e875">Irrigation is included in the current version of ORCHIDEE. The irrigation
requirement is estimated as the deficit of the available water of the
corresponding grid to the potential evapotranspiration. The irrigation
extracts water from the local grid first and then its neighboring grids if
necessary <xref ref-type="bibr" rid="bib1.bibx32" id="paren.90"/>. This solution is acceptable for most of
the humid regions at a 0.5<inline-formula><mml:math id="M34" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> resolution since the rivers are very
likely within 100 km. However, for dry regions, the Tarim for
example, the irrigation area is concentrated, with controlled irrigation
infrastructures. The nearby rivers are far from the irrigation area, and the
irrigated water is not taken directly from the rivers but transported from
upstream by channels. Due to the shortcoming of the scheme and the lack of
knowledge on the local irrigation, we turned off the irrigation in ORCHIDEE.
In the Tarim Basin, the irrigation accounts for more than 95 % of the
consumed water <xref ref-type="bibr" rid="bib1.bibx99" id="paren.91"/>, so that the difference between the simulated
discharge and observations can be attributed to neglecting irrigation in the
model.</p>
      <p id="d1e893">In conclusion, as shown in Fig. <xref ref-type="fig" rid="Ch1.F2"/>, four different forcing
inputs are prepared to drive the ORCHIDEE simulations, two basic forcing
datasets (WFD-CRU and WFDEI-CRU), one after correction by CMA (WFDEI-CMA) and then
one after adding glacier melt (WFDEI-CCG). Among them, the input water
amounts are different, while WFDEI-CMA and WFDEI-CCG have the same other
forcing variables as WFDEI-CRU. Additionally, the experiment with the
newly developed snow and soil freezing scheme is named WFDEI-CCG-SF based on the
forcing dataset WFDEI-CCG. Because the WFD covers the overlapping period
1901–2002, the WFDEI covers the period 1979–2014, CMA covers years
1951–2016 and the glacier melt dataset covers 1958–2001, all the
simulations and analysis in this paper are over the overlap period
1979–2001. The monthly discharge measurements for those chosen hydrological
gauges over 1979–2001 are then compiled. Spatial resolution for all the
forcing inputs remains 0.5<inline-formula><mml:math id="M35" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (about 50 km at the Equator), and the time
step is 3 h.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS3">
  <title>Main biases over the headwater catchments</title>
      <p id="d1e914">In the water cycle, all the water entering a specific river basin will become
ET back to the atmosphere and discharge (<inline-formula><mml:math id="M36" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>) flowing
out of the basin as long-term water storage changes are negligible. The
underestimation of discharge is thus attributable either to the
underestimation of water inputs or to overestimation of evapotranspiration. The
possible biases from water inputs and the ET estimation are discussed in this
section.</p><?xmltex \hack{\newpage}?>
<?pagebreak page6093?><sec id="Ch1.S3.SS3.SSS1">
  <title>Bias in precipitation</title>
      <p id="d1e930">The Tarim Basin is one of the areas where significant deviations exist among
different modeled precipitation estimates and observation-derived datasets
because of the sparse observations and orographic effects <xref ref-type="bibr" rid="bib1.bibx25 bib1.bibx82" id="paren.92"/>. Meanwhile, the precipitation bias might not be well addressed in the
CMA system because the number of meteorological gauges is still too limited
in the Tarim region to build a reliable interpolation climate field
<xref ref-type="bibr" rid="bib1.bibx64" id="paren.93"/>. Although <xref ref-type="bibr" rid="bib1.bibx83" id="text.94"/> have tried to use other gauges
outside China, the density of the gauge distribution is extremely low around
the boundaries of the Tarim Basin where most of the precipitation is
generated. Furthermore, due to the orographic effects, the precipitation over
the mountainous area is larger and with more significant heterogeneity than
that in the plains <xref ref-type="bibr" rid="bib1.bibx14 bib1.bibx4 bib1.bibx66" id="paren.95"/>, while the center of
the precipitation events is hard to observe for the nearby gauges.
<xref ref-type="bibr" rid="bib1.bibx1" id="text.96"/> has pointed out that the orography could cause 41.6 %
underestimation of the precipitation over the northwestern North American
mountainous ranges, and the deviations are larger at higher altitude.</p>
</sec>
<sec id="Ch1.S3.SS3.SSS2">
  <title>Bias in rainfall and snowfall repartition</title>
      <p id="d1e954">The differences between WFDEI-CRU and WFDEI-CMA are not only in the total
amount of precipitation but also in the proportion of rainfall and snowfall
(Table <xref ref-type="table" rid="Ch1.T3"/>). Compared to the rainfall, the snowfall is more
difficult to observe and affected by a large uncertainty; hence in the CMA
dataset, only the rainfall was recorded and then used to scale the CRU
dataset but keeping the relative proportion of liquid and solid precipitation
provided by WFDEI-CRU. The energy needs for phrases change are considerably
different for the liquid from the solid water. <xref ref-type="bibr" rid="bib1.bibx6" id="text.97"/>
suggested snow will lead to more runoff than rain in similar conditions based
on the observations over the US and China. The impact of the precipitation
type on the evapotranspiration rate is affected by many factors and hard to
measure.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p id="d1e965">Different formulas of Budyko curves. Note that the
aridity index is expressed as <inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:mi mathvariant="normal">∅</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> PET <inline-formula><mml:math id="M38" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M39" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>. </p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="142.26378pt"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">No.</oasis:entry>
         <oasis:entry colname="col2">Parameter</oasis:entry>
         <oasis:entry colname="col3">Formula</oasis:entry>
         <oasis:entry colname="col4">Reference</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">1</oasis:entry>
         <oasis:entry colname="col2">Non-parameter</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:mi mathvariant="normal">ET</mml:mi><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="normal">∅</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">
                        <xref ref-type="bibr" rid="bib1.bibx62" id="text.98"/>
                      </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">2</oasis:entry>
         <oasis:entry colname="col2">Non-parameter</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:mi mathvariant="normal">ET</mml:mi><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="normal">∅</mml:mi><mml:mi>tan⁡</mml:mi><mml:mi>h</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mi mathvariant="normal">∅</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">
                        <xref ref-type="bibr" rid="bib1.bibx49" id="text.99"/>
                      </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">3</oasis:entry>
         <oasis:entry colname="col2">Non-parameter</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:mi mathvariant="normal">ET</mml:mi><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mi mathvariant="normal">∅</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">
                        <xref ref-type="bibr" rid="bib1.bibx50" id="text.100"/>
                      </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">4</oasis:entry>
         <oasis:entry colname="col2">Non-parameter</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mi mathvariant="normal">ET</mml:mi><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:mo mathvariant="italic">{</mml:mo><mml:mo>[</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mi mathvariant="normal">∅</mml:mi></mml:mrow></mml:msup><mml:mo>]</mml:mo><mml:mo>⋅</mml:mo><mml:mi mathvariant="normal">∅</mml:mi><mml:mo>⋅</mml:mo><mml:mi>tanh⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mi mathvariant="normal">∅</mml:mi><mml:mo>)</mml:mo><mml:msup><mml:mo mathvariant="italic">}</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">
                        <xref ref-type="bibr" rid="bib1.bibx8" id="text.101"/>
                      </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">5</oasis:entry>
         <oasis:entry colname="col2">Parameter <inline-formula><mml:math id="M44" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:mi mathvariant="normal">ET</mml:mi><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mo>[</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mi mathvariant="normal">∅</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mi>n</mml:mi></mml:msup><mml:msup><mml:mo>]</mml:mo><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><xref ref-type="bibr" rid="bib1.bibx47" id="text.102"/>; <xref ref-type="bibr" rid="bib1.bibx12" id="text.103"/>; <xref ref-type="bibr" rid="bib1.bibx85" id="text.104"/></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">6</oasis:entry>
         <oasis:entry colname="col2">Parameter <inline-formula><mml:math id="M46" display="inline"><mml:mi mathvariant="italic">ϖ</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:mi mathvariant="normal">ET</mml:mi><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi mathvariant="normal">∅</mml:mi><mml:mo>-</mml:mo><mml:mo>[</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mo>(</mml:mo><mml:mi mathvariant="normal">∅</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mi mathvariant="italic">ϖ</mml:mi></mml:msup><mml:msup><mml:mo>]</mml:mo><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mi mathvariant="italic">ϖ</mml:mi></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">
                        <xref ref-type="bibr" rid="bib1.bibx27" id="text.105"/>
                      </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">7</oasis:entry>
         <oasis:entry colname="col2">Parameter <inline-formula><mml:math id="M48" display="inline"><mml:mi mathvariant="italic">ϖ</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:mi mathvariant="normal">ET</mml:mi><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ϖ</mml:mi><mml:mi mathvariant="normal">∅</mml:mi><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ϖ</mml:mi><mml:mi mathvariant="normal">∅</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mi mathvariant="normal">∅</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">
                        <xref ref-type="bibr" rid="bib1.bibx95" id="text.106"/>
                      </oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S3.SS3.SSS3">
  <title>Bias in glacier melt</title>
      <p id="d1e1473">HYOGA2 is a state-of-the-art global glacier model but has not been
calibrated over the Tarim Basin. The general bias for global estimation is
around <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5.0</mml:mn></mml:mrow></mml:math></inline-formula> % compared to the available global glacier mass balance
measurements <xref ref-type="bibr" rid="bib1.bibx37" id="paren.107"/>. The estimated annual glacier melt
amount is <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:mn mathvariant="normal">81.0</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M52" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for the whole Tarim Basin
(Table <xref ref-type="table" rid="Ch1.T3"/>), significantly lower than previous estimations
(<xref ref-type="bibr" rid="bib1.bibx90" id="altparen.108"/>: <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:mn mathvariant="normal">133.4</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M55" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M56" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>;
<xref ref-type="bibr" rid="bib1.bibx28" id="altparen.109"/>: <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:mn mathvariant="normal">144.16</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M59" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). On the one hand,
the difference in the forcing which drives the glacier melting model is
probably one of the causes of the deviation. On the other hand, all the
glacier melt is evenly distributed in a whole grid. It leads to a higher
infiltration ratio and thus feeds more evaporation <xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx54" id="paren.110"/>. This also artificially forces part of the glacier melt to flow
out of the grid not belonging to the right basin. However, it is unable to
eliminate this problem with the current gridded concepts. Finer spatial
resolution in glacier dataset and model simulation is needed to lessen the
impacts of discretization.</p>
</sec>
<sec id="Ch1.S3.SS3.SSS4">
  <title>Bias in potential evapotranspiration estimation</title>
      <p id="d1e1617">As described in Sect. 3.2.1, the PET estimation is independent of underlying
conditions (e.g., topography, vegetation) because enough water is provided. It
is therefore determined only by forcing conditions, especially the humidity
gradient and aerodynamic conditions (e.g., radiation flux, wind). Temperature
also plays a role in its estimation. Thus, the bias in PET is mainly
propagated from various forcing variables.</p>
</sec>
<sec id="Ch1.S3.SS3.SSS5">
  <title>Bias in actual evapotranspiration estimation</title>
      <p id="d1e1626">Overestimation (underestimation) of the actual ET will
also result in the discharge underestimation (overestimation). Many processes
can cause ET errors either by the biases in PET or the stress functions which
limit the potential evaporation. The vegetation fraction, vegetation type,
surface slope and soil properties are all the uncertain sources affecting the
final ET estimation.</p>
</sec>
<sec id="Ch1.S3.SS3.SSS6">
  <title>Bias sources category</title>
      <p id="d1e1635">With the main biases listed as above, we consider bias in any processes that
changes <inline-formula><mml:math id="M60" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> or PET as bias from forcing and bias in any processes that
directly changes ET as bias caused by model structure. Although the shifts in
forcing variables will change the ET estimation – for example, the <inline-formula><mml:math id="M61" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>
restricts the available water for ET – this shift still belongs to the
forcing category since the relation is indirect. The biases which directly
affect ET include biases in infiltration, soil water movement, snow
processes, vegetation representation and many other model processes. And all
these are considered as biases caused by model structures.</p>
</sec>
</sec>
<sec id="Ch1.S3.SS4">
  <title>Budyko hypothesis</title>
      <p id="d1e1659">Budyko hypothesis is an empirical expression for the coupling of the water
and energy balances at the surface. It uses the relation between the water
and energy balance equation to partition <inline-formula><mml:math id="M62" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> into
ET and <inline-formula><mml:math id="M63" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula>. The Budyko curve is the analytical
solution to the Budyko hypothesis, expressed as the evapotranspiration
rate (ET <inline-formula><mml:math id="M64" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M65" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) being a function of the aridity index (PET <inline-formula><mml:math id="M66" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M67" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>)
<xref ref-type="bibr" rid="bib1.bibx8" id="paren.111"/>. Many forms of Budyko curves have been developed and can
be categorized into a non-parameter group and parameter group depending on
whether there is an adjustable parameter describing the Budyko shape
(Table <xref ref-type="table" rid="Ch1.T1"/>).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2"><caption><p id="d1e1713">The definition of climate types by precipitation and
aridity index (<xref ref-type="bibr" rid="bib1.bibx53" id="altparen.112"/>).</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Climatic types</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M68" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Aridity index</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(mm yr<inline-formula><mml:math id="M69" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">(PET <inline-formula><mml:math id="M70" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M71" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Superarid</oasis:entry>
         <oasis:entry colname="col2">&lt; 100</oasis:entry>
         <oasis:entry colname="col3">&gt; 30</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Hyperarid</oasis:entry>
         <oasis:entry colname="col2">100–200</oasis:entry>
         <oasis:entry colname="col3">12–30</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Arid</oasis:entry>
         <oasis:entry colname="col2">200–400</oasis:entry>
         <oasis:entry colname="col3">5–12</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Semiarid</oasis:entry>
         <oasis:entry colname="col2">400–800</oasis:entry>
         <oasis:entry colname="col3">2–5</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Subhumid</oasis:entry>
         <oasis:entry colname="col2">800–1600</oasis:entry>
         <oasis:entry colname="col3">0.75–2</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Humid</oasis:entry>
         <oasis:entry colname="col2">1600–3200</oasis:entry>
         <oasis:entry colname="col3">0.375–0.75</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Hyperhumid</oasis:entry>
         <oasis:entry colname="col2">3200–6400</oasis:entry>
         <oasis:entry colname="col3">0.1875–0.375</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Superhumid</oasis:entry>
         <oasis:entry colname="col2">&gt; 6400</oasis:entry>
         <oasis:entry colname="col3">&lt; 0.1875</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?pagebreak page6094?><p id="d1e1887">The forms without parameters (formulas 1 to 4) are universal for most of the
basins, while they are unable to capture the various landscape
characteristics across regions <xref ref-type="bibr" rid="bib1.bibx84" id="paren.113"/>. Regarding the effects of
landscape characteristics, adjustable parameters and corresponding formulas
were introduced as formula (5) to (8). Although they have different analytical
expressions, the shape of these curves is quite similar <xref ref-type="bibr" rid="bib1.bibx29" id="paren.114"/>
and their parameters are highly correlated <xref ref-type="bibr" rid="bib1.bibx85" id="paren.115"/>. Hence, from the
formulas with parameters, Fu's equation (formula 6) is chosen in this
study as it is more often used in the China region.</p>
      <p id="d1e1899">The ranges of the aridity index (PET <inline-formula><mml:math id="M72" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M73" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) correspond to the regional
precipitation feeds and climate types (Table <xref ref-type="table" rid="Ch1.T2"/>). For
example, the precipitation for a semiarid region ranges from
400 to 800 mm yr<inline-formula><mml:math id="M74" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, and the regional aridity index mostly ranges
from 2 to 5. Moreover, the Budyko curve is a reflection of the landscape
characteristics which can influence the water movement through different
hydrological cycles <xref ref-type="bibr" rid="bib1.bibx18" id="paren.116"/> and thus changes the ET rate. Many
surface conditions are related to the Budyko parameter setting.
(1) Vegetation types and vegetation cover affect the ET rate. Transpiration accounts for about 42 % (25 %–64 %
depends on different models) of global ET <xref ref-type="bibr" rid="bib1.bibx96" id="paren.117"/>. Regions
that have a larger fraction of vegetation cover or are covered by vegetation with
bigger leaves and deeper roots tend to have a larger transpiration rate as well
as ET rate; i.e., the forested catchment tends to show a higher evaporation
ratio than the grass-covered catchments <xref ref-type="bibr" rid="bib1.bibx96 bib1.bibx9" id="paren.118"/>.
(2) Properties of soil determine infiltration rates and the amount of
evapotranspirable water. Steeper slopes are more likely to shed surface water
as runoff <xref ref-type="bibr" rid="bib1.bibx84 bib1.bibx94" id="paren.119"/>. Limit of infiltration ability also
matters as intense precipitation rates <xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx54" id="paren.120"/> or
freezing soils tend to force the water into the surface runoff (the solid
frozen soil limits the percolation of infiltrated water;
<xref ref-type="bibr" rid="bib1.bibx31" id="altparen.121"/>). (3) The ability to transmit or retain infiltrated
water of soil also determines the evapotranspiration rate; the soil with larger water conductivity is likely to release more
subsurface water rather than evaporation <xref ref-type="bibr" rid="bib1.bibx84" id="paren.122"/>. (4) The soil depth
determines the ability to store infiltrated water. Rocky mountains or regions
with thin soil would produce more runoff and less ET <xref ref-type="bibr" rid="bib1.bibx85 bib1.bibx18" id="paren.123"/>.</p>
</sec>
<sec id="Ch1.S3.SS5">
  <title>Bias assessment with the ORCHIDEE-Budyko framework</title>
      <p id="d1e1963">The Budyko formulation relates the ET to PET and <inline-formula><mml:math id="M75" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>. Both the biases from
the water flux (<inline-formula><mml:math id="M76" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) and energy flux (PET) will propagate to ET. The shape
parameter of the Budyko curve is obtained by fitting the PET <inline-formula><mml:math id="M77" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M78" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> and ET <inline-formula><mml:math id="M79" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M80" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>
relation; it is thus a reflection of the model if we use the simulated PET
and ET fluxes (i.e., ORCHIDEE simulations in this study, red dots and red
curve in Fig. <xref ref-type="fig" rid="Ch1.F3"/>). However, because of the existing bias
in all the three variables, the relations of the three components may have
been shifted to an unrealistic state (point A in
Fig. <xref ref-type="fig" rid="Ch1.F3"/>). Therefore, the changes in <inline-formula><mml:math id="M81" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, PET or ET
which can shift the system back to a reliable state are considered as the
possible bias. The difference between the unrealistic state with their
corrected values provides the estimation of how the forcing or the model
would need to be changed for the model to produce the realistic discharge
values. To separate the individual effect of the single water–energy
component on the hydrologic cycle, three independent assumptions are made as
follows, and the illustration can be found in Fig. <xref ref-type="fig" rid="Ch1.F3"/>.</p>
      <p id="d1e2022">The red dots in Fig. <xref ref-type="fig" rid="Ch1.F3"/> represent the states of the
PET <inline-formula><mml:math id="M82" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M83" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> and ET <inline-formula><mml:math id="M84" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M85" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> according to ORCHIDEE estimations and<?pagebreak page6095?> forcing inputs for
each year. Point A represents the representative state, which is the average
of the dots' locations. It reflects the current model and is probably in an
unrealistic state because the modeled discharge (<inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>-</mml:mo></mml:mrow></mml:math></inline-formula>ET) may be with bias
compared to the observations.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p id="d1e2068">The illustration of the ORCHIDEE-Budyko framework. Point A
represents the average state among the modeled annual values (with the land
surface model ORCHIDEE), and the red curve is the simulated Budyko curve
following the modeled state. Points B, C and D represent the representative state
with the <inline-formula><mml:math id="M87" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, PET and ET shifted, respectively, with different assumptions to
meet the discharge observations. A shifted Budyko curve (blue) is obtained
crossing the point D, which indicates a new state of the model structure. The
new points of B and C still stay on the original Budyko curve, indicating that
the model structure remains the same and the changes only relate to forcing
variables. The shaded area is the area among the three shifted states.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018-f03.pdf"/>

        </fig>

      <p id="d1e2084"><italic>Assumption 1.</italic> Only the water input (<inline-formula><mml:math id="M88" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) is uncertain. Because the
model structure remains unchanged, the relation between ET <inline-formula><mml:math id="M89" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M90" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> and
PET <inline-formula><mml:math id="M91" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M92" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> still follows the original Budyko line regardless of how <inline-formula><mml:math id="M93" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>
changes. The PET is assumed to be independent of <inline-formula><mml:math id="M94" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, while the ET is
modified as a result of <inline-formula><mml:math id="M95" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> changes. To meet the deviation between simulated
discharge (RS) and the observed discharge (RO), the representative point
(long-term “corrected” annual ET <inline-formula><mml:math id="M96" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M97" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> against long-term “corrected”
annual PET <inline-formula><mml:math id="M98" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M99" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) should be shifted along the Budyko curve from current
point “A” to the new point “B”, where the difference between the “true”
precipitation (<inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:msup><mml:mi>P</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>) and the “true” evapotranspiration (ET<inline-formula><mml:math id="M101" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>) equals the
observed discharge (<inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msup><mml:mi>P</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>-</mml:mo><mml:msup><mml:mi mathvariant="normal">ET</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> RO). The possible maximum bias in <inline-formula><mml:math id="M103" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>
is calculated as
            <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M104" display="block"><mml:mrow><mml:mi mathvariant="normal">bias</mml:mi><mml:mo>(</mml:mo><mml:mi>P</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mi>P</mml:mi><mml:mo>-</mml:mo><mml:msup><mml:mi>P</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:msup><mml:mi>P</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e2268"><italic>Assumption 2.</italic> Only the PET is uncertain. The <inline-formula><mml:math id="M105" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> remains the same, while ET
changes because of the changes in PET. Under these conditions, the model
structure still remains unchanged, and so does the Budyko curve. Then the
representative point should be shifted along the Budyko curve to point “C”
to decrease the ET ratio to meet the discharge observation (ET<inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:mi>P</mml:mi></mml:mrow></mml:math></inline-formula>-RO). The
PET is changed to a “true” PET<inline-formula><mml:math id="M107" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>, and the possible maximum bias in PET is
calculated as
            <disp-formula id="Ch1.E2" content-type="numbered"><mml:math id="M108" display="block"><mml:mrow><mml:mi mathvariant="normal">bias</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">PET</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mi mathvariant="normal">PET</mml:mi><mml:mo>-</mml:mo><mml:msup><mml:mi mathvariant="normal">PET</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:msup><mml:mi mathvariant="normal">PET</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e2348"><italic>Assumption 3.</italic> Only the ET is uncertain. <inline-formula><mml:math id="M109" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> and PET, which are mainly linked
to the forcing, remain the same, while the ET, which is significantly affected
by the model structure, is assumed biased. It is essentially relevant to the
model processes rather than the forcing dataset. To compensate the discharge
bias, the ET should be decreased to point “D” where the ET equals
precipitation minus observed discharge (ET'<inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mi>P</mml:mi><mml:mo>-</mml:mo></mml:mrow></mml:math></inline-formula>RO). The possible maximum
bias in ET is calculated as
            <disp-formula id="Ch1.E3" content-type="numbered"><mml:math id="M111" display="block"><mml:mrow><mml:mi mathvariant="normal">bias</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">ET</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mi mathvariant="normal">ET</mml:mi><mml:mo>-</mml:mo><mml:msup><mml:mi mathvariant="normal">ET</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:msup><mml:mi mathvariant="normal">ET</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="italic">%</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          With the target ET<inline-formula><mml:math id="M112" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>, a new Budyko curve can be drawn for new relations
between <inline-formula><mml:math id="M113" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, PET and the new ET (the blue lines in
Fig. <xref ref-type="fig" rid="Ch1.F3"/>). However, all the assumptions are proposed in
conditions of only one variable being uncertain, but in reality any of the
three variables can be biased at the same time. The final probable
“corrected” state may be located in the shaded area identified by the three
states (Fig. <xref ref-type="fig" rid="Ch1.F3"/>).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p id="d1e2441">The interannual cycle and intra-annual series of the precipitation
(including rainfall, snowfall and glacier) in difference simulations for the
upper Tarim Basin.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018-f04.pdf"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <title>Results and discussion</title>
<sec id="Ch1.S4.SS1">
  <title>Forcing and discharge comparison</title>
<sec id="Ch1.S4.SS1.SSS1">
  <title>Forcing input comparison among experiments</title>
      <p id="d1e2467">We specify <inline-formula><mml:math id="M114" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> as the sum of all the water inputs into the
system, which include the atmospheric water flux (in its liquid and solid
phases) and glacier melt. The precipitation for the three headwater
catchments and the upper Tarim is listed in Table <xref ref-type="table" rid="Ch1.T3"/> for each
simulation. The interannual variations and the intra-annual cycle of total
precipitation over upper Tarim Basin are plotted for different forcing in
Fig. <xref ref-type="fig" rid="Ch1.F4"/>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><caption><p id="d1e2484">The five simulations in this study and basic diagnostics
of the water inputs over three headwater catchments and the upper Tarim
Basin. Units: <inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M116" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M117" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1">Subbasins</oasis:entry>

         <oasis:entry colname="col2">Area (km<inline-formula><mml:math id="M118" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>)</oasis:entry>

         <oasis:entry colname="col3">Simulations</oasis:entry>

         <oasis:entry colname="col4">Precipitation</oasis:entry>

         <oasis:entry colname="col5">Rainfall</oasis:entry>

         <oasis:entry colname="col6">Snowfall</oasis:entry>

         <oasis:entry colname="col7">Glacier</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="4">Upper Yarkand</oasis:entry>

         <oasis:entry rowsep="1" colname="col2" morerows="4">55 637</oasis:entry>

         <oasis:entry colname="col3">WFD-CRU</oasis:entry>

         <oasis:entry colname="col4">80.19</oasis:entry>

         <oasis:entry colname="col5">11.16</oasis:entry>

         <oasis:entry colname="col6">69.03</oasis:entry>

         <oasis:entry colname="col7">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CRU</oasis:entry>

         <oasis:entry colname="col4">82.04</oasis:entry>

         <oasis:entry colname="col5">20.82</oasis:entry>

         <oasis:entry colname="col6">61.22</oasis:entry>

         <oasis:entry colname="col7">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CMA</oasis:entry>

         <oasis:entry colname="col4">117.73</oasis:entry>

         <oasis:entry colname="col5">92.35</oasis:entry>

         <oasis:entry colname="col6">25.38</oasis:entry>

         <oasis:entry colname="col7">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CCG</oasis:entry>

         <oasis:entry rowsep="1" colname="col4" morerows="1">141.21</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="1">104.09</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="1">25.38</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="1">11.74</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">WFDEI-CCG-SF</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="4">Upper Hotan</oasis:entry>

         <oasis:entry rowsep="1" colname="col2" morerows="4">34 557</oasis:entry>

         <oasis:entry colname="col3">WFD-CRU</oasis:entry>

         <oasis:entry colname="col4">31.83</oasis:entry>

         <oasis:entry colname="col5">6.63</oasis:entry>

         <oasis:entry colname="col6">25.20</oasis:entry>

         <oasis:entry colname="col7">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CRU</oasis:entry>

         <oasis:entry colname="col4">33.34</oasis:entry>

         <oasis:entry colname="col5">4.37</oasis:entry>

         <oasis:entry colname="col6">28.97</oasis:entry>

         <oasis:entry colname="col7">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CMA</oasis:entry>

         <oasis:entry colname="col4">82.71</oasis:entry>

         <oasis:entry colname="col5">72.13</oasis:entry>

         <oasis:entry colname="col6">10.58</oasis:entry>

         <oasis:entry colname="col7">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CCG</oasis:entry>

         <oasis:entry rowsep="1" colname="col4" morerows="1">137.34</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="1">99.45</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="1">10.58</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="1">27.31</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">WFDEI-CCG-SF</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="4">Upper Aksu</oasis:entry>

         <oasis:entry rowsep="1" colname="col2" morerows="4">31 982</oasis:entry>

         <oasis:entry colname="col3">WFD-CRU</oasis:entry>

         <oasis:entry colname="col4">76.11</oasis:entry>

         <oasis:entry colname="col5">49.06</oasis:entry>

         <oasis:entry colname="col6">27.05</oasis:entry>

         <oasis:entry colname="col7">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CRU</oasis:entry>

         <oasis:entry colname="col4">78.03</oasis:entry>

         <oasis:entry colname="col5">41.83</oasis:entry>

         <oasis:entry colname="col6">36.19</oasis:entry>

         <oasis:entry colname="col7">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CMA</oasis:entry>

         <oasis:entry colname="col4">106.38</oasis:entry>

         <oasis:entry colname="col5">72.22</oasis:entry>

         <oasis:entry colname="col6">34.16</oasis:entry>

         <oasis:entry colname="col7">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CCG</oasis:entry>

         <oasis:entry rowsep="1" colname="col4" morerows="1">120.23</oasis:entry>

         <oasis:entry rowsep="1" colname="col5" morerows="1">79.15</oasis:entry>

         <oasis:entry rowsep="1" colname="col6" morerows="1">34.15</oasis:entry>

         <oasis:entry rowsep="1" colname="col7" morerows="1">6.93</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col3">WFDEI-CCG-SF</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1" morerows="4">Upper Tarim</oasis:entry>

         <oasis:entry colname="col2" morerows="4">359 022</oasis:entry>

         <oasis:entry colname="col3">WFD-CRU</oasis:entry>

         <oasis:entry colname="col4">435.94</oasis:entry>

         <oasis:entry colname="col5">221.55</oasis:entry>

         <oasis:entry colname="col6">214.39</oasis:entry>

         <oasis:entry colname="col7">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CRU</oasis:entry>

         <oasis:entry colname="col4">473.31</oasis:entry>

         <oasis:entry colname="col5">246.35</oasis:entry>

         <oasis:entry colname="col6">226.96</oasis:entry>

         <oasis:entry colname="col7">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CMA</oasis:entry>

         <oasis:entry colname="col4">649.71</oasis:entry>

         <oasis:entry colname="col5">524.08</oasis:entry>

         <oasis:entry colname="col6">125.63</oasis:entry>

         <oasis:entry colname="col7">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CCG</oasis:entry>

         <oasis:entry colname="col4" morerows="1">758.74</oasis:entry>

         <oasis:entry colname="col5" morerows="1">578.60</oasis:entry>

         <oasis:entry colname="col6" morerows="1">125.62</oasis:entry>

         <oasis:entry colname="col7" morerows="1">54.52</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col3">WFDEI-CCG-SF</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e2922">The annual cycle of the two basic forcing datasets WFD-CRU and WFDEI-CRU are
similar, while the precipitation in WFDEI-CRU is slightly larger in monthly
values (Fig. <xref ref-type="fig" rid="Ch1.F4"/>a, red and blue lines). The deviation is the
result of their expanding differences after 1990 (Fig. <xref ref-type="fig" rid="Ch1.F4"/>b). The
precipitation difference is mainly due to the fact that two different versions of CRU
(CRU TS 2.10 and CRU TS 3.1) are used for precipitation correction in WFD and
WFDEI <xref ref-type="bibr" rid="bib1.bibx77" id="paren.124"><named-content content-type="pre">see Sect. 3.1.2 or</named-content></xref>. The precipitation difference
between the two CRU datasets is relatively small, while the CMA dataset increases
the precipitation to a large extent, by 37.3 %, compared to CRU for the
upper Tarim Basin (Table <xref ref-type="table" rid="Ch1.T3"/>). The changes mostly occur
during summer when the peak of CMA precipitation is more than twice as large
as precipitation in CRU. The shape of the annual cycle changes greatly
as the timing of the peak is shifted from April to July.<?pagebreak page6096?> However, the
precipitation amount in winter (DJF) decreases in CMA, to which the
decrease in snowfall is the major contributor. The changes in rainfall and
snowfall are similar in all three headwater catchments
(Table <xref ref-type="table" rid="Ch1.T3"/>) and the upper Tarim Basin.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><caption><p id="d1e2941">The temporal variations of the glacier melt, the proportion of
glacier melt in the water input and the average summer temperature over the
upper Tarim Basin. They are in good correlation and have a consistent
increasing trend after 1990.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018-f05.pdf"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p id="d1e2952">The interannual cycle and intra-annual series of the discharge
simulation for three headwater catchments and the upper Tarim Basin:
<bold>(a, b)</bold> Yarkand River, <bold>(c, d)</bold> Hotan River, <bold>(e, f)</bold> Aksu River and <bold>(g, h)</bold> the upper Tarim Basin. Observed
discharge for each subbasin was aggregated by the measurements at separated
discharge gauges and shown as the black solid line. The simulated discharges
at the corresponding grids were extracted from each experiment and plotted as
the color lines with markers. The dotted line and dot-dash line in the
interannual cycle plots represent the observed discharge in different
periods.</p></caption>
            <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018-f06.pdf"/>

          </fig>

      <p id="d1e2973">Adding the glacier melt leads to negligible changes during winter and spring
but large increases in the total water inputs in summer (JJA) when the
temperature is higher. The estimated glacier melt is 9.1 %, 25.8 %
and 6.1 % to the total water inputs for the upper Yarkand River, upper Hotan
River and upper Aksu River. It significantly increases after 1990
(Fig. <xref ref-type="fig" rid="Ch1.F5"/>; the trend is <inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">3.8</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M120" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M121" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>,
<inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.024</mml:mn></mml:mrow></mml:math></inline-formula>), being consistent with its ratio to the total water input
(<inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.918</mml:mn></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.001</mml:mn></mml:mrow></mml:math></inline-formula>). The trend is mainly caused by climate warming as the
glacier melt is highly correlated with the summer temperature (<inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:mi>r</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.852</mml:mn></mml:mrow></mml:math></inline-formula>,
<inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.001</mml:mn></mml:mrow></mml:math></inline-formula>). The increasing trend has also been documented in glacier runoff
observations <xref ref-type="bibr" rid="bib1.bibx63" id="paren.125"/>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4" specific-use="star"><caption><p id="d1e3080">The water–energy components for the headwater catchments
in WFDEI-CCG-SF simulation. Units: mm yr<inline-formula><mml:math id="M127" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="9">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Precipitation</oasis:entry>
         <oasis:entry colname="col3">Rainfall</oasis:entry>
         <oasis:entry colname="col4">Snowfall</oasis:entry>
         <oasis:entry colname="col5">Glacier</oasis:entry>
         <oasis:entry colname="col6">ET</oasis:entry>
         <oasis:entry colname="col7">RS</oasis:entry>
         <oasis:entry colname="col8">PET</oasis:entry>
         <oasis:entry colname="col9">RO</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Upper Yarkand</oasis:entry>
         <oasis:entry colname="col2">247.3</oasis:entry>
         <oasis:entry colname="col3">198.8</oasis:entry>
         <oasis:entry colname="col4">48.5</oasis:entry>
         <oasis:entry colname="col5">22.4</oasis:entry>
         <oasis:entry colname="col6">188.3</oasis:entry>
         <oasis:entry colname="col7">59.1</oasis:entry>
         <oasis:entry colname="col8">1240.4</oasis:entry>
         <oasis:entry colname="col9">140.4</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Upper Hotan</oasis:entry>
         <oasis:entry colname="col2">317.8</oasis:entry>
         <oasis:entry colname="col3">287.2</oasis:entry>
         <oasis:entry colname="col4">30.6</oasis:entry>
         <oasis:entry colname="col5">78.9</oasis:entry>
         <oasis:entry colname="col6">236.9</oasis:entry>
         <oasis:entry colname="col7">81.3</oasis:entry>
         <oasis:entry colname="col8">1153.7</oasis:entry>
         <oasis:entry colname="col9">118.9</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Upper Aksu</oasis:entry>
         <oasis:entry colname="col2">365.8</oasis:entry>
         <oasis:entry colname="col3">255.5</oasis:entry>
         <oasis:entry colname="col4">110.3</oasis:entry>
         <oasis:entry colname="col5">22.4</oasis:entry>
         <oasis:entry colname="col6">238.1</oasis:entry>
         <oasis:entry colname="col7">128.0</oasis:entry>
         <oasis:entry colname="col8">631.8</oasis:entry>
         <oasis:entry colname="col9">250.1</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S4.SS1.SSS2">
  <title>Assessment of the discharge estimations with observations</title>
      <p id="d1e3255">Evaluating the bias in precipitation over meteorological rain gauges is not
convincing as most gauges are located at lower altitude, which makes it
difficult to capture regional patterns<?pagebreak page6097?> as intensive precipitation occurs over
higher mountains. Instead, the discharge measurement can serve as a better
reference since it integrates the net water flux over the entire basin.
Therefore, driven by the forcing, ORCHIDEE was used to simulate the river
discharge and for comparison to in situ observations
(Fig. <xref ref-type="fig" rid="Ch1.F6"/>). The corresponding assessment using criteria for
the three headwater catchments are plotted in Fig. <xref ref-type="fig" rid="Ch1.F7"/>. For
the three headwater catchments where most of the discharge of the Tarim Basin
is generated, the discharge is significantly underestimated, with the
underestimation ratio reaching 90 % (Figs. <xref ref-type="fig" rid="Ch1.F6"/>b, d, f,
<xref ref-type="fig" rid="Ch1.F7"/>a) for CRU datasets. Discharge increases after the
precipitation is corrected by the CMA dataset, with the absolute bias decreasing
to around 80 %. Adding glacier melt also increases the discharge but by
a relatively small amount. Changes in the model structure (new snow and soil
freezing scheme) further decrease the bias, especially for the Aksu River. The
final biases of the discharge for the three subbasins are <inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">71.1</mml:mn></mml:mrow></mml:math></inline-formula> %,
<inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">47.8</mml:mn></mml:mrow></mml:math></inline-formula> % and <inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">49.4</mml:mn></mml:mrow></mml:math></inline-formula> %. The gradual improvements and
corresponding magnitude changes are visible in the annual discharge
variability in Fig. <xref ref-type="fig" rid="Ch1.F6"/>b, d and f.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T5" specific-use="star"><caption><p id="d1e3302">The annual average values for different water–energy
components (<inline-formula><mml:math id="M131" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, ET, PET; units: mm yr<inline-formula><mml:math id="M132" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) and their relations
(<inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>-</mml:mo></mml:mrow></mml:math></inline-formula>ET, PET <inline-formula><mml:math id="M134" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M135" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> and ET <inline-formula><mml:math id="M136" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M137" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) for the three upstream subbasins. The scenarios
correspond to the diagnostics of the current model (A) and three bias
assumptions listed above from B to D. The bold values are the main factors
changed within the three basic water–energy components. The changing ratio
indicates the ratio of the changing value to the original value (unit: %),
while the bias range implies the bias of the values in the current
variables compared to the values they should be (unit: %). </p></caption><oasis:table frame="topbot"><oasis:tgroup cols="11">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="center"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:colspec colnum="8" colname="col8" align="right"/>
     <oasis:colspec colnum="9" colname="col9" align="left"/>
     <oasis:colspec colnum="10" colname="col10" align="right"/>
     <oasis:colspec colnum="11" colname="col11" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1"/>

         <oasis:entry colname="col2"/>

         <oasis:entry colname="col3"><inline-formula><mml:math id="M138" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4">PET</oasis:entry>

         <oasis:entry colname="col5">ET</oasis:entry>

         <oasis:entry colname="col6"><inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>-</mml:mo></mml:mrow></mml:math></inline-formula>ET</oasis:entry>

         <oasis:entry colname="col7">PET <inline-formula><mml:math id="M140" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M141" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col8">ET <inline-formula><mml:math id="M142" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M143" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col9">Factor</oasis:entry>

         <oasis:entry colname="col10">Changing ratio</oasis:entry>

         <oasis:entry colname="col11">Bias range</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="3">Upper Yarkand</oasis:entry>

         <oasis:entry colname="col2">A</oasis:entry>

         <oasis:entry colname="col3">247.3</oasis:entry>

         <oasis:entry colname="col4">1240.4</oasis:entry>

         <oasis:entry colname="col5">188.3</oasis:entry>

         <oasis:entry colname="col6">59.0</oasis:entry>

         <oasis:entry colname="col7">5.02</oasis:entry>

         <oasis:entry colname="col8">0.76</oasis:entry>

         <oasis:entry colname="col9">–</oasis:entry>

         <oasis:entry colname="col10">–</oasis:entry>

         <oasis:entry colname="col11">-</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">B</oasis:entry>

         <oasis:entry colname="col3"><bold>435.4</bold></oasis:entry>

         <oasis:entry colname="col4">1240.4</oasis:entry>

         <oasis:entry colname="col5"><bold>294.9</bold></oasis:entry>

         <oasis:entry colname="col6">140.5</oasis:entry>

         <oasis:entry colname="col7">2.85</oasis:entry>

         <oasis:entry colname="col8">0.68</oasis:entry>

         <oasis:entry colname="col9"><inline-formula><mml:math id="M144" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col10">76.1 %</oasis:entry>

         <oasis:entry colname="col11"><inline-formula><mml:math id="M145" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">43.2</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">C</oasis:entry>

         <oasis:entry colname="col3">247.3</oasis:entry>

         <oasis:entry colname="col4"><bold>225.0</bold></oasis:entry>

         <oasis:entry colname="col5"><bold>106.9</bold></oasis:entry>

         <oasis:entry colname="col6">140.4</oasis:entry>

         <oasis:entry colname="col7">0.91</oasis:entry>

         <oasis:entry colname="col8">0.43</oasis:entry>

         <oasis:entry colname="col9">PET</oasis:entry>

         <oasis:entry colname="col10"><inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">81.9</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>

         <oasis:entry colname="col11">451.2 %</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">D</oasis:entry>

         <oasis:entry colname="col3">247.3</oasis:entry>

         <oasis:entry colname="col4">1240.4</oasis:entry>

         <oasis:entry colname="col5"><bold>106.9</bold></oasis:entry>

         <oasis:entry colname="col6">140.4</oasis:entry>

         <oasis:entry colname="col7">5.02</oasis:entry>

         <oasis:entry colname="col8">0.43</oasis:entry>

         <oasis:entry colname="col9">ET</oasis:entry>

         <oasis:entry colname="col10"><inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">43.2</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>

         <oasis:entry colname="col11">76.1 %</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="3">Upper Hotan</oasis:entry>

         <oasis:entry colname="col2">A</oasis:entry>

         <oasis:entry colname="col3">317.8</oasis:entry>

         <oasis:entry colname="col4">1153.7</oasis:entry>

         <oasis:entry colname="col5">236.9</oasis:entry>

         <oasis:entry colname="col6">80.9</oasis:entry>

         <oasis:entry colname="col7">3.63</oasis:entry>

         <oasis:entry colname="col8">0.75</oasis:entry>

         <oasis:entry colname="col9">–</oasis:entry>

         <oasis:entry colname="col10">–</oasis:entry>

         <oasis:entry colname="col11">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">B</oasis:entry>

         <oasis:entry colname="col3"><bold>402.3</bold></oasis:entry>

         <oasis:entry colname="col4">1153.7</oasis:entry>

         <oasis:entry colname="col5"><bold>283.3</bold></oasis:entry>

         <oasis:entry colname="col6">119.0</oasis:entry>

         <oasis:entry colname="col7">2.85</oasis:entry>

         <oasis:entry colname="col8">0.70</oasis:entry>

         <oasis:entry colname="col9"><inline-formula><mml:math id="M148" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col10">26.6 %</oasis:entry>

         <oasis:entry colname="col11"><inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">21.0</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">C</oasis:entry>

         <oasis:entry colname="col3">317.8</oasis:entry>

         <oasis:entry colname="col4"><bold>615.2</bold></oasis:entry>

         <oasis:entry colname="col5"><bold>198.8</bold></oasis:entry>

         <oasis:entry colname="col6">118.9</oasis:entry>

         <oasis:entry colname="col7">1.94</oasis:entry>

         <oasis:entry colname="col8">0.63</oasis:entry>

         <oasis:entry colname="col9">PET</oasis:entry>

         <oasis:entry colname="col10"><inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">46.7</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>

         <oasis:entry colname="col11">87.5 %</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">D</oasis:entry>

         <oasis:entry colname="col3">317.8</oasis:entry>

         <oasis:entry colname="col4">1153.7</oasis:entry>

         <oasis:entry colname="col5"><bold>198.8</bold></oasis:entry>

         <oasis:entry colname="col6">118.9</oasis:entry>

         <oasis:entry colname="col7">3.63</oasis:entry>

         <oasis:entry colname="col8">0.63</oasis:entry>

         <oasis:entry colname="col9">ET</oasis:entry>

         <oasis:entry colname="col10"><inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">16.1</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>

         <oasis:entry colname="col11">19.1 %</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1" morerows="3">Upper Aksu</oasis:entry>

         <oasis:entry colname="col2">A</oasis:entry>

         <oasis:entry colname="col3">365.8</oasis:entry>

         <oasis:entry colname="col4">631.8</oasis:entry>

         <oasis:entry colname="col5">238.1</oasis:entry>

         <oasis:entry colname="col6">127.7</oasis:entry>

         <oasis:entry colname="col7">1.73</oasis:entry>

         <oasis:entry colname="col8">0.65</oasis:entry>

         <oasis:entry colname="col9">–</oasis:entry>

         <oasis:entry colname="col10">–</oasis:entry>

         <oasis:entry colname="col11">–</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">B</oasis:entry>

         <oasis:entry colname="col3"><bold>553.3</bold></oasis:entry>

         <oasis:entry colname="col4">631.8</oasis:entry>

         <oasis:entry colname="col5"><bold>303.1</bold></oasis:entry>

         <oasis:entry colname="col6">250.2</oasis:entry>

         <oasis:entry colname="col7">1.14</oasis:entry>

         <oasis:entry colname="col8">0.55</oasis:entry>

         <oasis:entry colname="col9"><inline-formula><mml:math id="M152" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col10">51.3 %</oasis:entry>

         <oasis:entry colname="col11"><inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">33.9</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">C</oasis:entry>

         <oasis:entry colname="col3">365.8</oasis:entry>

         <oasis:entry colname="col4"><bold>174.1</bold></oasis:entry>

         <oasis:entry colname="col5"><bold>115.7</bold></oasis:entry>

         <oasis:entry colname="col6">250.1</oasis:entry>

         <oasis:entry colname="col7">0.48</oasis:entry>

         <oasis:entry colname="col8">0.32</oasis:entry>

         <oasis:entry colname="col9">PET</oasis:entry>

         <oasis:entry colname="col10"><inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">72.4</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>

         <oasis:entry colname="col11">262.4 %</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">D</oasis:entry>

         <oasis:entry colname="col3">365.8</oasis:entry>

         <oasis:entry colname="col4">631.8</oasis:entry>

         <oasis:entry colname="col5"><bold>115.7</bold></oasis:entry>

         <oasis:entry colname="col6">250.1</oasis:entry>

         <oasis:entry colname="col7">1.73</oasis:entry>

         <oasis:entry colname="col8">0.32</oasis:entry>

         <oasis:entry colname="col9">ET</oasis:entry>

         <oasis:entry colname="col10"><inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">51.4</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>

         <oasis:entry colname="col11">105.8 %</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T6" specific-use="star"><caption><p id="d1e4006">Summary of the possible causes of the underestimation in
discharge and the corresponding arguments. Three levels of the possibility
are presented: yes: with direct argument; likely: with indirect argument; and
no: with negative argument.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="113.811024pt"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="170.716535pt"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1">Subbasin</oasis:entry>

         <oasis:entry colname="col2">Variable</oasis:entry>

         <oasis:entry colname="col3">Is it a factor?</oasis:entry>

         <oasis:entry colname="col4">Is it the only factor?</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="2">Upper Yarkand</oasis:entry>

         <oasis:entry rowsep="1" colname="col2"><inline-formula><mml:math id="M156" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> underestimation</oasis:entry>

         <oasis:entry rowsep="1" colname="col3">Yes: glacier (low glacier ratio, smaller trend in discharge simulation)</oasis:entry>

         <oasis:entry rowsep="1" colname="col4">Likely no (very high PET <inline-formula><mml:math id="M157" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1240.4 mm yr<inline-formula><mml:math id="M158" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; high ET<inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 0.68)</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">PET overestimation</oasis:entry>

         <oasis:entry colname="col3">Likely yes: very high <?xmltex \hack{\hfill\break}?>PET <inline-formula><mml:math id="M160" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1240.4 mm yr<inline-formula><mml:math id="M161" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4">No (very low PET <inline-formula><mml:math id="M162" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 225.0 mm yr<inline-formula><mml:math id="M163" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; low PET<inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 0.91)</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">ET overestimation</oasis:entry>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4">Likely no (very high PET <inline-formula><mml:math id="M165" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1240.4 mm yr<inline-formula><mml:math id="M166" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; high PET<inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 5.02)</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="2">Upper Hotan</oasis:entry>

         <oasis:entry rowsep="1" colname="col2"><inline-formula><mml:math id="M168" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> underestimation</oasis:entry>

         <oasis:entry rowsep="1" colname="col3"/>

         <oasis:entry rowsep="1" colname="col4">Likely no (very high PET <inline-formula><mml:math id="M169" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1153.7 mm yr<inline-formula><mml:math id="M170" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; high ET<inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 0.70)</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">PET overestimation</oasis:entry>

         <oasis:entry colname="col3">Likely yes: very high PET <inline-formula><mml:math id="M172" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1153.7 mm yr<inline-formula><mml:math id="M173" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>

         <oasis:entry colname="col4"/>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">ET overestimation</oasis:entry>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4">Likely no (very high PET <inline-formula><mml:math id="M174" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1153.7 mm yr<inline-formula><mml:math id="M175" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1" morerows="2">Upper Aksu</oasis:entry>

         <oasis:entry rowsep="1" colname="col2"><inline-formula><mml:math id="M176" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> underestimation</oasis:entry>

         <oasis:entry rowsep="1" colname="col3">Yes: <inline-formula><mml:math id="M177" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>&lt;</mml:mo><mml:mi>R</mml:mi></mml:mrow></mml:math></inline-formula> in summer</oasis:entry>

         <oasis:entry rowsep="1" colname="col4">Likely no (low PET<inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 1.14)</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">PET overestimation</oasis:entry>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4">No (very low PET <inline-formula><mml:math id="M179" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 174.1 mm yr<inline-formula><mml:math id="M180" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, very low PET<inline-formula><mml:math id="M181" display="inline"><mml:mrow><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 0.48)</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">ET overestimation</oasis:entry>

         <oasis:entry colname="col3"/>

         <oasis:entry colname="col4"/>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><caption><p id="d1e4412">The discharge diagnostics of different experiments for three
catchments (round – Yarkand; square – Hotan; and triangle – Aksu).
<bold>(a)</bold> represents the absolute bias in percentage,
<bold>(b)</bold> represents the correlation of the interannual cycle and
<bold>(c)</bold> represents the ratio of the trend in estimated discharge to that
in observed discharge for the period 1990–2001. S0 to S4 correspond to the
experiments WFD-CRU, WFDEI-CRU, WFDEI-CMA, WFDEI-CCG and WFDEI-CCG-SF
in ascending order.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018-f07.pdf"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><caption><p id="d1e4432">The water input components (rainfall, snowfall, glacier melt),
evapotranspiration and discharge for three headwater catchments (from top to bottom: <bold>a</bold>,
Yarkand; <bold>c</bold>, Hota; and <bold>e</bold>, Aksu) in the WFDEI-CCG-SF
simulation. In the left panels, the amounts of different variables are
plotted as bars, while the average mean of the observed discharge (RO) is
plotted as the red line. RS denotes the simulated discharge by ORCHIDEE. In
the right panels, the annual cycle of the water inputs (blue line),
evapotranspiration (green shadow), estimated discharge (runoff plus drainage,
solid black line), observed discharge (dashed black line) and changes in
terrestrial water storage (TWS, slashed area) are plotted as <bold>b</bold>, <bold>d</bold> and
<bold>f</bold>. The green slashed area represents decreasing in TWS, and the white
slashed area represents increasing in TWS.</p></caption>
            <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018-f08.pdf"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p id="d1e4462">Budyko relation for three headwater catchments (<bold>a</bold>, Yarkand;
<bold>b</bold>, Hotan; <bold>c</bold> Aksu). The red points represent the values for each year; the <inline-formula><mml:math id="M182" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> is
obtained from the forcing, while ET and PET are obtained from the model.
Point A represents the long-term average Budyko relation, and red lines are
the optimal fitted Budyko line. The water input <inline-formula><mml:math id="M183" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, the potential
evapotranspiration PET or the actual evapotranspiration ET can be modified to
meet the observed discharge, which correspondingly shifts the representative
points from A to B, C or D. B and C stay in the original Budyko curve, while a
new optimal fitted Budyko curve through point D can be built after the
changes in ET. The shaded area is the most likely area when not only a single
variable is changing.</p></caption>
            <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/6087/2018/hess-22-6087-2018-f09.pdf"/>

          </fig>

      <p id="d1e4494">Besides the increase in the annual mean discharge, the amplitude of the
interannual cycle of the discharge is also improved by the progressive
changes. The estimated discharge peaks have been shifted from April in CRU
simulations to the summer (July or August) by CMA correction and adding
glaciers (Fig. <xref ref-type="fig" rid="Ch1.F6"/>a, c, e). Correspondingly, the correlation
of the annual variability between the estimated and observed discharge has
increased above 0.9 for all the three subbasins with the WFDEI-CCG forcing
(Fig. <xref ref-type="fig" rid="Ch1.F7"/>b). However, contrary to the upper Yarkand River and the
upper Hotan River, the introduction of the new snow and soil freezing scheme
decreases the discharge correlation for the upper Aksu River from 0.91 to 0.42. An
early discharge peak exists in May, while not enough runoff is generated in
the summer period (Fig. <xref ref-type="fig" rid="Ch1.F6"/>e). Although the correlation
decreases, it does not mean the model/simulation deteriorates because
correlation only evaluates the similarity of temporal variation but ignores
the fact that the discharge amount has been better estimated
(Figs. <xref ref-type="fig" rid="Ch1.F6"/>e and <xref ref-type="fig" rid="Ch1.F7"/>a).</p>
      <p id="d1e4507">By extracting the observed discharge in the first and last 5 years from the
whole period, we can notice there is an obvious shift of the discharge peak
from August to July in the three headwater catchments
(Fig. <xref ref-type="fig" rid="Ch1.F6"/>a, c, e). The regional precipitation changes largely
cause the shift, but the increasing temperature also allows the snow/glacier
to melt at a higher rate in the most recent period. Furthermore, increasing
trends are detected after the 1990s (Fig. <xref ref-type="fig" rid="Ch1.F6"/>b, d, f), as the
increasing trend is <inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.43</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M185" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M186" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> (or
<inline-formula><mml:math id="M187" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.77</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M188" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M189" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.78</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M191" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M192" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>) for
the upper Yarkand (or Hotan, Aksu) River. The increasing trends are consistent with
the glacier melt, glacier proportion in water input and summer
temperature in the same period (Fig. <xref ref-type="fig" rid="Ch1.F5"/>).</p>
      <p id="d1e4618">The trends in the estimated discharge are also calculated and compared with
the observed trends, expressed as the ratio of the trend in estimation to
that in observations (Fig. <xref ref-type="fig" rid="Ch1.F7"/>c). For CRU simulations, no
increasing trend is detected since the ratio is less than 0. The CMA
correction increases the ratio for all three subbasins to around 0.3, which
means the precipitation accounts for only around 30 % of the discharge
increase. Adding the glacier melt increases the ratio from 0.35 to 0.54 for the upper Hotan River
and from 0.31 to 0.76 for the upper Aksu River; the improvement of
the glacier melting is comparable to the CMA correction. However, no
apparent changes are detected for the upper Yarkand River. By comparing the
criteria between WFDEI-CMA and WFDEI-CCG, we find that, although adding the
glacier melt does not change much the absolute amount of discharge or the
correlation, the increased trend in discharge has been considerably improved.
The increasing glacier melt is, therefore, one of the contributors to the
discharge trend in the Tarim. The modification of the snow and soil freezing
scheme increases the trend ratio in the upper Aksu River up to 0.72, while slightly
decreasing it for the two other catchments.</p>
      <p id="d1e4623">In brief, the gradual refinement of the forcing datasets (from WFD-CRU to
WFDEI-CRU to WFDEI-CMA to WFDEI-CCG) is effective for improving the model
performance using different criteria (bias, correlation, proportion to the
trend) to compare the observed discharge. The three criteria are independent
as they stand for the averages, the variation and the trend, which can
capture the various aspects of the model agreement to the observations. The
responses<?pagebreak page6099?> are similar for different catchments, but at different magnitude at
different stages. The correction of the CMA dataset is the most significant
improvement to all the criteria. The role of glaciers melting is critical for
the trend analysis. The modification in the snow and soil freezing scheme
increases the total discharge amount but could lead to adverse responses in
the correlation and trend simulation. However, the impact of the modification
of the model structure is not larger than changes resulting from the forcing
biases. From the previous analysis, we can conclude that the simulations of
WFDEI-CCG and WFDEI-CCG-SF are comparable in the correlation and trend
analysis, while WFDEI-CCG-SF is better regarding the water quantity.
Therefore, the further study on the bias is all based on the WFDEI-CCG-SF
simulation.</p>
</sec>
</sec>
<?pagebreak page6101?><sec id="Ch1.S4.SS2">
  <title>Evidence of the bias in estimated discharge for the headwater catchments</title>
      <p id="d1e4633">Although the simulations with WFDEI-CCG-SF are better than other experiments,
there are still biases compared to the observations
(Fig. <xref ref-type="fig" rid="Ch1.F7"/>a). In this section, we aim to find evidence of
the biases. The annual mean water balance components (rainfall, snowfall,
glacier melt, estimated ET and discharge RS) of the three upper catchments
are plotted as bars with their relations quantified by comparison to the
discharge observations (RO, red lines in Fig. <xref ref-type="fig" rid="Ch1.F8"/>a, c, e) in
WFDEI-CCG-SF. Their annual cycles are also plotted as Fig. <xref ref-type="fig" rid="Ch1.F8"/>b,
d and f over the three headwater catchments. Over a long enough period, the
changes in terrestrial water storage are assumed negligible compared to the
water fluxes, so that the water input into the system either returns to the
atmosphere through ET or flows out of the basin as RS.</p>
      <p id="d1e4642">From the left panels of the Fig. <xref ref-type="fig" rid="Ch1.F8"/>, we have a visual
impression of the relative amount of different water inputs and their
contribution to the ET or discharge. Note that the sum of the ET and RS is
not exactly equal to <inline-formula><mml:math id="M193" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> because in ORCHIDEE the discharge is represented at
the outflow of the grid and not at the confluence point of the analyzed
catchment with other tributaries. The largest bias is 8 % for the upper
Yarkand River (Fig. <xref ref-type="fig" rid="Ch1.F8"/>a, ET <inline-formula><mml:math id="M194" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M195" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M196" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> RS<inline-formula><mml:math id="M197" display="inline"><mml:mrow><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.92</mml:mn></mml:mrow></mml:math></inline-formula>), while it
matches exactly for the upper Aksu River. The bias can be added to the current RS
if necessary.</p>
      <p id="d1e4692">Among the three headwater catchments, the upper Hotan River has the best discharge
simulation compared to the observations (RS <inline-formula><mml:math id="M198" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> RO <inline-formula><mml:math id="M199" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.52</mml:mn></mml:mrow></mml:math></inline-formula>). The annual cycle of
the water also matches well as all the <inline-formula><mml:math id="M200" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, ET and discharge RO or RS
have the synchronous peaks in summer (Fig. <xref ref-type="fig" rid="Ch1.F8"/>d). There are also
deviations between <inline-formula><mml:math id="M201" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M202" display="inline"><mml:mi>E</mml:mi></mml:math></inline-formula>, which represent the net water inputs to the
system and the estimated discharge (the shaded area with blue lines in
Fig. <xref ref-type="fig" rid="Ch1.F8"/>d). The deviation implies the regional water storage
changes; in summer the soil moisture increases to store the abundant water
inputs, which are later released in autumn and winter when the drainage rate is
larger than infiltration. The water storage decreases as a result by
then. It is the natural adjustment to the strong seasonality in water inputs.</p>
      <p id="d1e4738">As the neighboring catchment of the upper Hotan River, the upper Yarkand River has
similar phases of estimated flux ratios (ET <inline-formula><mml:math id="M203" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> PET, ET <inline-formula><mml:math id="M204" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M205" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, RS <inline-formula><mml:math id="M206" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M207" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) and
interannual variations. However, the estimated discharge rate is
smaller (RS <inline-formula><mml:math id="M208" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> RO <inline-formula><mml:math id="M209" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M210" display="inline"><mml:mn mathvariant="normal">0.29</mml:mn></mml:math></inline-formula>) than that of the upper Hotan River. Underestimation in water
inputs in summer and autumn is possibly the reason as there is no obvious
water storage gaining in the summer period and the ratio of observed
discharge to regional precipitation is unrealistically high (<inline-formula><mml:math id="M211" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.9</mml:mn></mml:mrow></mml:math></inline-formula>,
Fig. <xref ref-type="fig" rid="Ch1.F8"/>b).</p>
      <?pagebreak page6102?><p id="d1e4811">The upper Aksu River has different characteristics from the other two regions since
it lies in the northern part of the Tarim. It has a larger snowfall
proportion in the precipitation. Meanwhile, it has the largest ratio of
estimated ET <inline-formula><mml:math id="M212" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> PET, the largest runoff generation ratio (RS<inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.35</mml:mn></mml:mrow></mml:math></inline-formula>) and
the least discharge simulation error (RS <inline-formula><mml:math id="M214" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> RO <inline-formula><mml:math id="M215" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.51). However,
there is certainly large bias in the regional precipitation as the discharge
has exceeded the precipitation input in the summer period (July and August).
The estimated annual cycle of discharge diverges from the observations
(Fig. <xref ref-type="fig" rid="Ch1.F8"/>f), as its peak advances by 2 months and the
discharge estimation significantly exceeds the observations in spring (MAM).
The runoff generation ratio in the summer period is also unrealistically low.</p>
      <p id="d1e4851">In summary, the biases in discharge estimation exist in terms of the total
amount and the annual cycle. Precipitation is one of the largest bias sources,
which makes the bias analysis in models more difficult.</p>
</sec>
<sec id="Ch1.S4.SS3">
  <title>Bias range and possibility analysis for the headwater catchments</title>
      <p id="d1e4860">Although either <inline-formula><mml:math id="M216" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> or PET or ET can cause final underestimation of discharge
over the three headwater catchments, quantifying the bias in each flux is
challenging and impractical due to the lack of direct measurements and the
strong heterogeneity over the mountainous area. To separate the individual
bias, we use the Budyko hypothesis by assuming only one variable is
uncertain, while the other two are assumed to have negligible errors, with
which we “correct” the model simulation to meet the discharge observation
and obtain the possible bias range. Then we evaluate the possibility of
rejecting the assumption to find the most likely bias source by checking the
status of the water system (i.e., amount of the water–energy components and
their relations) in indirect ways. The water–energy components used in the
Budyko analysis are all ORCHIDEE outputs of the most satisfactory simulation,
WFDEI-CCG-SF. The corresponding characteristics of the water–energy
components for three headwater catchments are listed in
Table <xref ref-type="table" rid="Ch1.T4"/>.</p>
<sec id="Ch1.S4.SS3.SSS1">
  <title>Bias ranges estimated by the ORCHIDEE-Budyko framework</title>
      <p id="d1e4877">The ORCHIDEE-estimated evapotranspiration rate (ET <inline-formula><mml:math id="M217" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M218" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) against the estimated
aridity index (PET <inline-formula><mml:math id="M219" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M220" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) over each subbasin in each year is scattered as red
points in Fig. <xref ref-type="fig" rid="Ch1.F9"/>. Point A represents the Budyko relation
between long-term average annual ET <inline-formula><mml:math id="M221" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M222" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> and the long-term average annual
PET <inline-formula><mml:math id="M223" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M224" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>. According to the categories introduced by <xref ref-type="bibr" rid="bib1.bibx53" id="text.126"/>, all
three catchments belong to semiarid climate zones by the definition of the
annual average precipitation (Table <xref ref-type="table" rid="Ch1.T2"/>). Hence the
aridity index is supposed to range from 2 to 5. Regarding the high
elevation and cold temperature, the PET rate is likely to be smaller than the
representative climate of this aridity index. Thus the aridity index for the
three catchments is supposed to be lower than expected. It is realistic for the
upper Hotan River and the upper Aksu River as their aridity is 3.63 and 1.73,
respectively. While the aridity index for the upper Yarkand River is 5.02, which can
be categorized as a semiarid or arid region, this is not very likely since the
upper Yarkand River is providing water resources for the irrigated area over the
lower Yarkand oases <xref ref-type="bibr" rid="bib1.bibx99 bib1.bibx46" id="paren.127"/>.</p>
      <p id="d1e4948">However, because there is still a bias in the ORCHIDEE discharge estimations
with the observations, the current state A is not correct. Based on the
assumptions introduced in Sect. 3.5, the three possible “corrected” states
by shifting the <inline-formula><mml:math id="M225" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, PET and ET are shown in Fig. <xref ref-type="fig" rid="Ch1.F9"/>
for the three headwater catchments. Taking the upper Yarkand River as an example
(Fig. <xref ref-type="fig" rid="Ch1.F9"/>a), if we consider only <inline-formula><mml:math id="M226" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> to be biased (assumption 1), the
<inline-formula><mml:math id="M227" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> has to be shifted from 247.3 to 435.4 mm yr<inline-formula><mml:math id="M228" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. PET remains the
same, and the ET changes accordingly, but the relation between ET <inline-formula><mml:math id="M229" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M230" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> and
PET <inline-formula><mml:math id="M231" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M232" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> still follows the Budyko curve. The state is shifted from point A to
point B with the <inline-formula><mml:math id="M233" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> change ratio as 76.1 %. Reversely, the possible bias
of <inline-formula><mml:math id="M234" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> is <inline-formula><mml:math id="M235" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">43.2</mml:mn></mml:mrow></mml:math></inline-formula> % ((247.3–435.4)<inline-formula><mml:math id="M236" display="inline"><mml:mrow><mml:mo>/</mml:mo><mml:mn mathvariant="normal">435.4</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> %). Similarly, to change the PET in
order to shift the state to correct (point C, assumption 2), the PET has to
be shifted from 1240.4 to 225.0 mm yr<inline-formula><mml:math id="M237" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The possible bias in PET is
451.2 %. To change the ET in order to shift the state to correct (point
D, assumption 3), the ET has to be shifted from 188.3  to
106.9 mm yr<inline-formula><mml:math id="M238" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, and the possible bias in ET is 76.1 %. The route is
the same for the other two catchments, and their results are listed in
Table <xref ref-type="table" rid="Ch1.T5"/>.</p>
      <p id="d1e5082">The previous analysis is based on the assumptions that the <inline-formula><mml:math id="M239" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> and
PET are independent and only a single variable is uncertain, which might be
invalid in reality. However, the three assumptions provide the bias
boundaries of each variable, and the final system reproducing observed RO is
likely to be located within the shaded area shown in Fig. <xref ref-type="fig" rid="Ch1.F9"/>.
Taking the Hotan River as an example, to meet the discharge observation, the final
changes in <inline-formula><mml:math id="M240" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> will be 0 %–26.6 %, the decrease in PET will be
0 %–46.7 % and the decrease in ET will range 0 %–16.1 %.
While in turn, we also conclude that the <inline-formula><mml:math id="M241" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> is underestimated by
0 %–21.0 %, the PET is overestimated by 87.5 % at most and the
ET is overestimated by 19.1 % at most. If we know the bias for any single
variable, the feasible ranges will be narrower than at present.</p>
</sec>
<sec id="Ch1.S4.SS3.SSS2">
  <title>Ranking the bias possibility</title>
      <p id="d1e5114">Although the Budyko approach provides us with possible ranges for the bias of
each variable, it is still difficult to determine the bias source without
proper bias measurements for each of the forcing variables. We alternatively
compare the regional diagnostics with nearby regions or regions with similar
climatic and regional characteristics which have qualified observations in an
indirect way. In doing so, we can generally rank the occurrence possibility
of an uncertain variable.</p>
      <?pagebreak page6103?><p id="d1e5117">From multiple-model analysis based on CMIP5 general circulation models (GCMs), the estimated PET over the
western boundary of the Tarim Basin is about the same as over the
Tibetan Plateau <xref ref-type="bibr" rid="bib1.bibx61" id="paren.128"/>. However, because of the unpredictable
biases in GCMs, the absolute values are not highly reliable in their
simulation. Nevertheless, the equivalent relation provides us with the ranges of
PET over the Tarim headwater catchments by referring to the observations over
the Tibetan Plateau, where the topography changes are relatively small and the
observations are more abundant. According to <xref ref-type="bibr" rid="bib1.bibx10" id="text.129"/>, who used site
observations from 101 stations over the Tibetan Plateau, the annual average PET
over the plateau ranges from 580 to 720 mm yr<inline-formula><mml:math id="M242" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Hence the PET over the
upper Yarkand River and the upper Hotan River is probably overestimated (1240.4 and
1153.7 mm yr<inline-formula><mml:math id="M243" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). Therefore, only changes in <inline-formula><mml:math id="M244" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> or ET are not
satisfactory because the PET is unchanged. For the upper Yarkand River, the
PET is not the only error source, because, to match the discharge deviation by
only decreasing PET, the PET should be decreased to 225 mm yr<inline-formula><mml:math id="M245" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, which
exceeds the referenced PET range. Moreover, because Yarkand and Hotan are
neighboring regions which have similar climates, the PET should be a
similar amount in each (615.2 mm yr<inline-formula><mml:math id="M246" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> if only PET is uncertain in the upper Hotan River,
while 225 mm yr<inline-formula><mml:math id="M247" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in the Yarkand River). The estimated PET over the Aksu River is
realistic since the PET is 631.8 mm yr<inline-formula><mml:math id="M248" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for the current scenario, but
it would decrease to 174.1 mm yr<inline-formula><mml:math id="M249" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> if only the PET changed, which
is too low. Besides the absolute value of PET, the ratio PET <inline-formula><mml:math id="M250" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M251" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> also shifts
when PET changes, which means the climatic types can be changed. Only
decreasing the PET in the upper Yarkand and the upper Aksu River would cause
significant decreases in the aridity index (from 5.02 to 0.91 for the upper
Yarkand, from 1.73 to 0.48 for the upper Aksu River), which are not realistic for
these regions.</p>
      <p id="d1e5233">ET computation is sensitive to the climatic conditions and the surface
conditions; hence the absolute value of ET significantly varies in time and
space, and its bias very difficult to quantify. The evapotranspiration
ratio to precipitation (ET <inline-formula><mml:math id="M252" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M253" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) is typical for specific climatic types or
regions with similar land cover types <xref ref-type="bibr" rid="bib1.bibx84" id="paren.130"/>. <xref ref-type="bibr" rid="bib1.bibx43" id="text.131"/>
estimated the evapotranspiration ratio to precipitation using a remote-sensing
approach over regions of Canada. They concluded that the ratio ET <inline-formula><mml:math id="M254" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M255" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> is
32 % for barren land and 18 % for snow/ice land. In general, most of
the catchment area of the three headwater catchments consists of barren and
snow/ice land. Because of its lower latitude, the ET ratio could be
higher but still below the rate for cropland (67 %). Therefore, only
changes in <inline-formula><mml:math id="M256" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> are not very likely for Yarkand and Hotan (ET <inline-formula><mml:math id="M257" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M258" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> is 0.68 for
Yarkand and 0.70 for Hotan after the correction). Higher <inline-formula><mml:math id="M259" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> for the
upper Aksu River is likely to maintain a realistic ET <inline-formula><mml:math id="M260" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M261" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> ratio.</p>
      <p id="d1e5314">The biases of the three variables (<inline-formula><mml:math id="M262" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, ET, PET) have relatively weak
dependence because they are governed by different processes. <inline-formula><mml:math id="M263" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> and PET are
quite independent because they relate to different forcing variables.
Although the ET amount is linked to two other variables, the ET bias is
weakly dependent, and it also comes more from the surface conditions and model
biases. The chances of biases arising from each variable are about the same
in theory. However, based on the analysis of the model output and the assumed
bias-corrected scenarios, there are some priorities for the bias sources over
each subbasin. The possibility of biases and the supporting arguments are
listed in Table <xref ref-type="table" rid="Ch1.T6"/> for each headwater catchment. For
instance, for the upper Yarkand subbasin, an increase in <inline-formula><mml:math id="M264" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, especially the
glacier melt, is necessary because of the lower glacier melt ratio compared to
the Hotan basin (Sect. 5.1.2.3) and the small trend in model discharge
compared to the discharge observation (Sect. 4.2). However, only increasing
the precipitation is not sufficient because the current PET is very likely
too high compared to the surrounding regions (PET <inline-formula><mml:math id="M265" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1240.4 mm yr<inline-formula><mml:math id="M266" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>,
while PET ranges 580–720 mm yr<inline-formula><mml:math id="M267" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> over the Tibetan Plateau). Meanwhile,
only decreasing the PET without changing other variables would cause a very low PET rate
(225 mm yr<inline-formula><mml:math id="M268" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) and low aridity index (PET<inline-formula><mml:math id="M269" display="inline"><mml:mrow><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo></mml:mrow></mml:math></inline-formula> 0.91), which is not
realistic for this region. Modification in ET is possible but not adequate
due to the overestimated PET. Hence, this error analysis reveals that
increasing precipitation over the upper Yarkand subbasin is quite necessary,
the overestimation of PET is very likely and modification in ET estimation
is possible but not fundamentally necessary. For the upper Hotan River, the most
likely biases come from the overestimation of PET, while the two other
variables are possible sources. An increase in precipitation and changes in temporal
variability are necessary for the upper Aksu subbasin, but they are not the
only causes, as either the PET or ET, or both, is overestimated.</p>
</sec>
</sec>
<sec id="Ch1.S4.SS4">
  <title>Human intervention in the lower oases</title>
      <p id="d1e5403">The current ORCHIDEE version does not yet take into account the intensified
evapotranspiration caused by human activities especially through irrigation,
which is a major process in the hydrological cycle transferring water to the
atmosphere. As a consequence, in the lower oases the simulated discharge at
the Alar station is significantly larger than the observations
(Fig. <xref ref-type="fig" rid="Ch1.F6"/>g, h; <inline-formula><mml:math id="M270" display="inline"><mml:mrow><mml:mn mathvariant="normal">146.59</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M271" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M272" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in
WFDEI-CCG-SF simulation to <inline-formula><mml:math id="M273" display="inline"><mml:mrow><mml:mn mathvariant="normal">43.34</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M274" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M275" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> in
observation). However, because the biases of the upstream discharge will
propagate to the Alar station, the catchment of which includes the three
basins discussed above, the currently estimated discharge is thus
underestimated compared to the potential river flow at Alar, which is the
natural river flow without human intervention.</p>
      <p id="d1e5481">We use two simple approaches to estimate this underestimation. In the first one,
according to the work of <xref ref-type="bibr" rid="bib1.bibx69" id="text.132"/>, all the water increment of the
Alar gauge station is caused by the water changes from the three headwater
catchments. Hence the underestimation of the discharge to the potential river
flow at Alar equals the underestimation<?pagebreak page6104?> of discharge from those three
catchments. The increment at Alar should be <inline-formula><mml:math id="M276" display="inline"><mml:mrow><mml:mn mathvariant="normal">110.25</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M277" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M278" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (observed <inline-formula><mml:math id="M279" display="inline"><mml:mrow><mml:mn mathvariant="normal">192.15</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M280" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M281" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>
from the three headwater catchments minus simulated <inline-formula><mml:math id="M282" display="inline"><mml:mrow><mml:mn mathvariant="normal">81.9</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M283" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M284" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), so that the potential river flow at Alar should
be <inline-formula><mml:math id="M285" display="inline"><mml:mrow><mml:mn mathvariant="normal">256.84</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M286" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M287" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (<inline-formula><mml:math id="M288" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">146.59</mml:mn><mml:mo>+</mml:mo><mml:mn mathvariant="normal">110.25</mml:mn></mml:mrow></mml:math></inline-formula>), and the
influence of human activities on the increase of ET can be estimated as
<inline-formula><mml:math id="M289" display="inline"><mml:mrow><mml:mn mathvariant="normal">213.50</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M290" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M291" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (<inline-formula><mml:math id="M292" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">256.84</mml:mn><mml:mo>-</mml:mo><mml:mn mathvariant="normal">43.34</mml:mn></mml:mrow></mml:math></inline-formula>), 83.1 % of
discharge.</p>
      <p id="d1e5698">A second simple scaling approach to obtaining the potential river flow at
Alar is that we assume the model bias for the whole
upper Tarim Basin is constant over space. The scaling factor is 2.35
(<inline-formula><mml:math id="M293" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">192.15</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">81.9</mml:mn></mml:mrow></mml:math></inline-formula>); hence the potential discharge at Alar should be
<inline-formula><mml:math id="M294" display="inline"><mml:mrow><mml:mn mathvariant="normal">343.92</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M295" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M296" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (=<inline-formula><mml:math id="M297" display="inline"><mml:mrow><mml:mn mathvariant="normal">146.59</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">2.35</mml:mn></mml:mrow></mml:math></inline-formula>). And the
influence of human activities on the increase of ET is estimated as
<inline-formula><mml:math id="M298" display="inline"><mml:mrow><mml:mn mathvariant="normal">300.58</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M299" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M300" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>(<inline-formula><mml:math id="M301" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">343.92</mml:mn><mml:mo>-</mml:mo><mml:mn mathvariant="normal">43.34</mml:mn></mml:mrow></mml:math></inline-formula>), 87.4 % of the
discharge. The overestimation over the discharge observation is the amount
caused by additional human intervention, especially the irrigation-caused
evapotranspiration.</p>
      <p id="d1e5814">To validate the proposed values, we collected the irrigation area over the
Tarim Basin using the FAO Global Map of Irrigation Areas <xref ref-type="bibr" rid="bib1.bibx67" id="paren.133"/>,
according to which the total irrigated area for the upper Tarim Basin is
13 548.5 km<inline-formula><mml:math id="M302" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>. In addition, <xref ref-type="bibr" rid="bib1.bibx99" id="text.134"/> provides the gross
irrigation quota as <inline-formula><mml:math id="M303" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.77</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">6</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M304" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> km<inline-formula><mml:math id="M305" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; hence the total
irrigation water consumption will be <inline-formula><mml:math id="M306" display="inline"><mml:mrow><mml:mn mathvariant="normal">239.80</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M307" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M308" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.
Hence the results of the two approaches assessing human net abstraction are
<inline-formula><mml:math id="M309" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">11</mml:mn></mml:mrow></mml:math></inline-formula> % and 25 % (<inline-formula><mml:math id="M310" display="inline"><mml:mrow><mml:mn mathvariant="normal">213.50</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M311" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M312" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and
<inline-formula><mml:math id="M313" display="inline"><mml:mrow><mml:mn mathvariant="normal">300.58</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">8</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> m<inline-formula><mml:math id="M314" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msup></mml:math></inline-formula> yr<inline-formula><mml:math id="M315" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, respectively) in relation to
the consumption data, which are acceptable figures because of the unknown biases in
irrigation area as well as the gross irrigation quota. The proportion of the
consumed water (83.1 %–87.4 %) is higher than the estimation
(74.7 %) in 1995, which could be explained by the intra-annual variation
of inflow and abstraction.</p>
</sec>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusions</title>
      <p id="d1e5996">In this work, we proposed an ORCHIDEE-Budyko framework which is used to
attribute the modeled discharge bias to different sources as the forcing and
model structure. Bias in the precipitation (<inline-formula><mml:math id="M316" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>) and any processes related to
the potential evapotranspiration (PET) is considered as bias from forcing and
bias in any processes affecting the actual evapotranspiration (ET) estimation
is considered as bias from model structures. The discharge simulation was
provided by the land surface model ORCHIDEE with latest developments in its
modules and driven by the most improved forcing inputs (WFDEI-CCG-SF).
However, underestimation in the discharge still exists over the three Tarim
headwater catchments, where the biases of <inline-formula><mml:math id="M317" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula>, PET and ET are analyzed with a
Budyko analytical approach. With a set of assumptions, we isolated the biases
in three variables, and their possibilities were assessed with information
from nearby and hydroclimatically similar regions. Results show that
precipitation (here considered as the sum of rainfall, snowfall and glacier
melt) underestimation is highly likely for the upper Yarkand River and the upper
Aksu River, while the overestimation of PET is likely to affect the upper Yarkand
River and the upper Hotan River. The overestimation in ET is possible but not likely the
only cause for the discharge underestimation for all headwater catchments. In
the lower oases, humans consume 83.1 %–87.4 % of the discharge for
irrigation, which is also a bias source in the current version of model. Thus,
inclusion of detailed human modules is needed for any large-scale model.</p>
      <p id="d1e6013">In this attempt to analyze the performance of a complex land surface model
over the Tarim Basin, large biases are found in the discharge estimation. Our
finding that the bias is most likely caused by the forcing variables rather
than the model is probably the reason for the failures of other models in
specific regions as well. Our work provides more information about the Tarim
Basin's water cycle and guidance for future studies that the bias in forcing
variables should firstly be assessed and reduced in order to perform
pertinent analysis of the regional water cycle. Land surface models are a
recommended tool for water cycle analysis because of their independence of
calibration and good ability to simulate most variables of the water cycle
and their interplay, which facilitates the identification of bias sources.
This kind of application along with the improvements of forcing data is also
important for predicting water resources in the Tarim as well as other
high-altitude basins in central Asia in a changing climate.</p>
</sec>

      
      </body>
    <back><notes notes-type="codedataavailability">

      <p id="d1e6020">The land surface model is free to download on the
website
<uri>https://forge.ipsl.jussieu.fr/orchidee/browser/branches/publications/ORCHIDEE_gmd-2018-57</uri>
(<xref ref-type="bibr" rid="bib1.bibx48" id="altparen.135"/>). The WFD dataset can be obtained from
<uri>http://www.waterandclimatechange.eu/about/watch-forcing-data-20th-century</uri>
(<xref ref-type="bibr" rid="bib1.bibx75" id="altparen.136"/>). The WFDEI dataset can be obtained from
<uri>http://www.eu-watch.org/gfx_content/documents/README-WFDEI (v2016).pdf</uri>
(<xref ref-type="bibr" rid="bib1.bibx78" id="altparen.137"/>). The CRU datasets are available through
<uri>http://catalogue.ceda.ac.uk/uuid/ac3e6be017970639a9278e64d3fd5508</uri>
(<xref ref-type="bibr" rid="bib1.bibx40" id="altparen.138"/>). The CMA dataset is available through website
<uri>http://data.cma.cn/data/detail/dataCode/SURF_CLI_CHN_PRE_MON_GRID_0.5/</uri>
(<xref ref-type="bibr" rid="bib1.bibx98" id="altparen.139"/>).</p>
  </notes><notes notes-type="authorcontribution">

      <p id="d1e6057">JP initialized the ideas presented in this paper with XZ
and TY. XZ prepared the simulations, the figures and the manuscript.
TY and YH participated in the data preparation. TNQ
participated in the model development. All authors contributed to the discussion
and revising the paper.</p>
  </notes><notes notes-type="competinginterests">

      <p id="d1e6063">The authors declare that they have no conflict of
interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e6069">This study was supported by the National Natural Science Foundation of China
(grant nos. 41561134016 and 51879068); the CHINA-TREND-STREAM French national project (ANR grant no.
ANR-15-CE01-00L1-0L); the National Key Research and Development
Program (2018YFC0407900); the Global Environmental Research Fund (S-14) of
the Ministry of the Environment, Japan; and the China Scholarship Council
(CSC, 201506710042). The work was supported by computing resource of the IPSL
ClimServ cluster at École Polytechnique, France. We also thank the
editor and the anonymous reviewers for their contribution to the improvement
of this paper. <?xmltex \hack{\newline}?><?xmltex \hack{\newline}?> Edited by: Zhongbo Yu
<?xmltex \hack{\newline}?> Reviewed by: three anonymous referees</p></ack><ref-list>
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    <!--<article-title-html>Understanding the water cycle over the upper Tarim Basin: retrospecting the estimated discharge bias to atmospheric variables and model structure</article-title-html>
<abstract-html><p>The bias in atmospheric variables and that in model computation are
two major causes of failures in discharge estimation. Attributing the bias in
discharge estimation becomes difficult if the forcing bias cannot be
evaluated and excluded in advance in places lacking qualified meteorological
observations, especially in cold and mountainous areas (e.g., the upper
Tarim Basin). In this study, we proposed an Organizing Carbon and Hydrology In Dynamic
EcosystEms (ORCHIDEE)-Budyko framework which
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structure) with a set of analytical approaches. The latest version of the land
surface model ORCHIDEE was used to provide reliable discharge simulations
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assumptions. Results show that, as the forcing biases, the water inputs
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Tarim headwater catchments (−43.2&thinsp;% to 21.0&thinsp;%). Meanwhile, the
potential evapotranspiration is unrealistically high over the upper Yarkand
and the upper Hotan River (1240.4 and 1153.7&thinsp;mm&thinsp;yr<sup>−1</sup>, respectively). Determined by the model structure, the bias in actual
evapotranspiration is possible but not the only contributor to the discharge
underestimation (overestimated by up to 105.8&thinsp;% for the upper Aksu River). Based
on a simple scaling approach, we estimated the water consumption by human
intervention ranging from 213.50×10<sup>8</sup>  to
300.58×10<sup>8</sup>&thinsp;m<sup>3</sup>&thinsp;yr<sup>−1</sup> at the Alar gauge station, which is
another bias source in the current version of ORCHIDEE. This study succeeded
in retrospecting the bias from the discharge estimation to multiple bias
sources of the atmospheric variables and the model structure. The framework
provides a unique method for evaluating the regional water cycle and its
biases with our current knowledge of observational uncertainties.</p></abstract-html>
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