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<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0" article-type="methods-article">
  <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-26-4575-2022</article-id><title-group><article-title>Technical note: Do different projections matter for the<?xmltex \hack{\break}?> Budyko framework?</article-title><alt-title>Budyko framework: do different projections matter?</alt-title>
      </title-group><?xmltex \runningtitle{Budyko framework: do different projections matter?}?><?xmltex \runningauthor{R.~C.~Nijzink and S.~J.~Schymanski}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes">
          <name><surname>Nijzink</surname><given-names>Remko C.</given-names></name>
          <email>remko_nijzink@live.nl</email>
        <ext-link>https://orcid.org/0000-0002-9999-9883</ext-link></contrib>
        <contrib contrib-type="author" corresp="no">
          <name><surname>Schymanski</surname><given-names>Stanislaus J.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0950-2942</ext-link></contrib>
        <aff id="aff1"><institution>Catchment and Ecohydrology Group (CAT), Environmental Research and Innovation (ERIN),<?xmltex \hack{\break}?> Luxembourg Institute of Science and Technology (LIST), Belvaux, Luxembourg</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Remko C. Nijzink (remko_nijzink@live.nl)</corresp></author-notes><pub-date><day>14</day><month>September</month><year>2022</year></pub-date>
      
      <volume>26</volume>
      <issue>17</issue>
      <fpage>4575</fpage><lpage>4585</lpage>
      <history>
        <date date-type="received"><day>6</day><month>April</month><year>2022</year></date>
           <date date-type="accepted"><day>20</day><month>August</month><year>2022</year></date>
           <date date-type="rev-recd"><day>12</day><month>July</month><year>2022</year></date>
           <date date-type="rev-request"><day>20</day><month>April</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 Remko C. Nijzink</copyright-statement>
        <copyright-year>2022</copyright-year>
      <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/26/4575/2022/hess-26-4575-2022.html">This article is available from https://hess.copernicus.org/articles/26/4575/2022/hess-26-4575-2022.html</self-uri><self-uri xlink:href="https://hess.copernicus.org/articles/26/4575/2022/hess-26-4575-2022.pdf">The full text article is available as a PDF file from https://hess.copernicus.org/articles/26/4575/2022/hess-26-4575-2022.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d1e91">The widely used Budyko framework defines the water and energy limits of catchments. Generally, catchments plot close to these physical limits, and
<xref ref-type="bibr" rid="bib1.bibx6" id="text.1"/> developed a curve that predicted the positions of catchments in this framework. Often, the independent variable is
defined as an aridity index, which is used to predict the ratio of actual evaporation over precipitation (<inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi></mml:mrow></mml:math></inline-formula>). However, the framework
can be formulated with the potential evaporation as the common denominator for the dependent and independent variables, i.e., <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. It is possible to mathematically convert between these formulations, but if the parameterized Budyko curves are fit to
data, the different formulations could lead to differences in the resulting parameter values. Here, we tested this for 357 catchments across the
contiguous United States.</p>

      <p id="d1e145">In this way, we found that differences in <inline-formula><mml:math id="M4" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values due to the projection used could be <inline-formula><mml:math id="M5" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2. If robust fitting algorithms were used, the
differences in <inline-formula><mml:math id="M6" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values reduced but were nonetheless still present. The distances to the curve, often used as a metric in Budyko-type analyses,
systematically depended on the projection, with larger differences for the non-contracted sides of the framework (i.e., <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> or
<inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>). When using the two projections for predicting <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, we found that uncertainties due to the projections used could
exceed 1.5 %. An important reason for the differences in <inline-formula><mml:math id="M10" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values, curves and resulting estimates of <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> could be found in
data points that clearly appear as outliers in one projection but less so in the other projection.</p>

      <p id="d1e237">We argue here that the non-contracted side of the framework in the two projections should always be assessed, especially for data points that appear
as outliers. At least, one should consider the additional uncertainty of the projection and assess the robustness of the results in both
projections.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e249"><xref ref-type="bibr" rid="bib1.bibx6" id="text.2"/> defined the water and energy limits of catchments in a simple framework and found that most catchments plot close to
these limits. He defined a curve through these observations, which is known as the Budyko curve. The framework and curve are widely applied, and the
original work of <xref ref-type="bibr" rid="bib1.bibx6" id="text.3"/> has been cited over 3100 times (Google Scholar). Besides that, Budyko's approach finds itself currently
in a renaissance, as can be noted by the large number of studies related to the Budyko framework over the recent years. The strength of the approach
is widely acknowledged, and especially its simplicity is appealing.</p>
      <p id="d1e257">Even though often referred to as the Budyko framework, the base of the framework was formed by the work of <xref ref-type="bibr" rid="bib1.bibx30" id="text.4"/> and
<xref ref-type="bibr" rid="bib1.bibx37" id="text.5"/>. Initially, <xref ref-type="bibr" rid="bib1.bibx37" id="text.6"/> formulated an exponential function to calculate the runoff ratio of a catchment
but only as a function of precipitation and a constant, catchment-specific parameter. <xref ref-type="bibr" rid="bib1.bibx30" id="text.7"/> added evaporation to this
equation but also formulated his own hyperbolic tangent function. <xref ref-type="bibr" rid="bib1.bibx6" id="text.8"/> took later the arithmetic mean of the exponential
function and the hyperbolic tangent function, which both had no parameters, to adjust the curve. This was changed by <xref ref-type="bibr" rid="bib1.bibx39" id="text.9"/> in France
and independently in the Soviet Union by <xref ref-type="bibr" rid="bib1.bibx22" id="text.10"/>, who both introduced an adjustable exponent. This parameterized form was adopted
later by others, in more general formulations, e.g., <xref ref-type="bibr" rid="bib1.bibx14" id="text.11"/>, <xref ref-type="bibr" rid="bib1.bibx49" id="text.12"/>, and <xref ref-type="bibr" rid="bib1.bibx35" id="text.13"/>. These
formulations often use one single parameter to adjust the curve to the observations. See also <xref ref-type="bibr" rid="bib1.bibx3" id="text.14"/> for more details
about the historical perspective.</p>
      <p id="d1e294">More recently, the Budyko framework has gained popularity with several studies that use the framework for water balance assessment
<xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx8" id="paren.15"><named-content content-type="pre">e.g., </named-content></xref>, model constraining
<xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx18 bib1.bibx23 bib1.bibx17" id="paren.16"><named-content content-type="pre">e.g., </named-content></xref> or the assessment of climate change
effects <xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx5" id="paren.17"><named-content content-type="pre">e.g., </named-content></xref>. In addition, several studies exist that adjust the framework for
different timescales <xref ref-type="bibr" rid="bib1.bibx50 bib1.bibx41" id="paren.18"/> or different application fields <xref ref-type="bibr" rid="bib1.bibx36" id="paren.19"/>.</p>
      <p id="d1e318">A large number of studies consider the parameter in the Budyko framework to be catchment-specific and a function of local catchment characteristics. It
has been argued that this parameter explains local climatic and environmental conditions combined <xref ref-type="bibr" rid="bib1.bibx35" id="paren.20"><named-content content-type="pre">e.g., </named-content></xref>, but it is
often also related to vegetation <xref ref-type="bibr" rid="bib1.bibx44 bib1.bibx20 bib1.bibx29" id="paren.21"><named-content content-type="pre">e.g., </named-content></xref>, land cover <xref ref-type="bibr" rid="bib1.bibx31" id="paren.22"/> or
human activities <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx47" id="paren.23"/>. Moreover, <xref ref-type="bibr" rid="bib1.bibx49" id="text.24"/> defined <inline-formula><mml:math id="M12" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> specifically as the plant-available water coefficient. In addition to vegetation, <xref ref-type="bibr" rid="bib1.bibx11" id="text.25"/> related the parameter to multiple variables including storm depths
and soil water storage capacities. Furthermore, seasonality is often considered as well as a factor that influences this parameter
<xref ref-type="bibr" rid="bib1.bibx38 bib1.bibx29" id="paren.26"/>.</p>
      <p id="d1e355">Budyko formulated his curve with an aridity index as the independent variable, and most other publications followed that definition. From the older
and traditionally cited publications, only <xref ref-type="bibr" rid="bib1.bibx39" id="text.27"/> and <xref ref-type="bibr" rid="bib1.bibx32" id="text.28"/> formulated the framework with potential
evaporation as the common denominator and <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> as the independent variable <xref ref-type="bibr" rid="bib1.bibx4" id="paren.29"/>. Nowadays, most publications
still use a form of the Budyko framework with the dryness or aridity index <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi></mml:mrow></mml:math></inline-formula> to predict the dependent variable <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi></mml:mrow></mml:math></inline-formula>,
similar as Budyko, but a substantial number of papers use <inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> as an independent variable to predict the ratio of
<inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. Here we refer to these different ways of expressing the dependent and independent variables in the Budyko framework as
dryness index and wetness index projections, respectively. These two projections are only discussed in combination in very few studies
<xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx33" id="paren.30"><named-content content-type="pre">e.g., </named-content></xref>.</p>
      <p id="d1e451">The choice of the projection may depend on the purpose of a given study. Often, the projection with an aridity index is used as it allows for a
straightforward estimation of the runoff ratio (<inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:mi>Q</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:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi></mml:mrow></mml:math></inline-formula>), which can, for example, be used directly for constraining hydrological
models <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx18" id="paren.31"><named-content content-type="pre">e.g., </named-content></xref>. In contrast, assessing responses to changes in precipitation may require
a projection that uses <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> as the predicted variable <xref ref-type="bibr" rid="bib1.bibx12" id="paren.32"><named-content content-type="pre">e.g., </named-content></xref>, in order to allow for a clearer
interpretation of sensitivities. Others use the different projections simultaneously, for example, to identify gaining or leaky catchments
<xref ref-type="bibr" rid="bib1.bibx2" id="paren.33"/>. However, a large number of studies use the projection based on an aridity index, most likely just following the
definition of the framework by <xref ref-type="bibr" rid="bib1.bibx6" id="text.34"/>, without questioning the appropriateness of this projection.</p>
      <p id="d1e516">Generally, the projections should not make a large difference, as the equations can be rewritten in the different formats <xref ref-type="bibr" rid="bib1.bibx35" id="paren.35"><named-content content-type="pre">see, for example,
</named-content></xref>, but here we argue that this does matter in case the curve is fit to observations. Moreover, these different ways of
defining the Budyko space may lead to different interpretations of deviations from the curve. Therefore, we explore here the consequences of the
projection used and address the following research question: does the choice of the projection and fitting algorithm have a systematic influence on the curve parameter, uncertainties, distances of individual
catchments to the curve or distances of individual catchments to the physical limits?</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Methodology</title>
      <p id="d1e532">In order to address the research question, the Budyko framework was applied to a selection of catchments across the contiguous United States. An open
science approach was followed using the platform Renku (<uri>https://renkulab.io/</uri>, last access: 30 March 2022), which stores all data, scripts and
analyses as well as the linkage between these elements. An online repository contains all information necessary for reproducibility and repeatability
(<uri>https://renkulab.io/projects/remko.nijzink/budyko</uri>; <xref ref-type="bibr" rid="bib1.bibx27" id="altparen.36"/>), with the final figures and latex files in a separate repository
(<uri>https://renkulab.io/gitlab/remko.nijzink/budyko_tech_note</uri>, last access: 4 April 2022).</p>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Budyko formulations</title>
      <p id="d1e554">The Budyko formulation adopted for our analysis was originally formulated by <xref ref-type="bibr" rid="bib1.bibx22" id="text.37"/> <xref ref-type="bibr" rid="bib1.bibx45" id="paren.38"><named-content content-type="pre">as traced back by </named-content></xref>
but used afterwards by, amongst others, <xref ref-type="bibr" rid="bib1.bibx7" id="text.39"/> and <xref ref-type="bibr" rid="bib1.bibx35" id="text.40"/>:
            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M20" display="block"><mml:mrow><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mrow><mml:mrow><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:msup><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi>n</mml:mi></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi>n</mml:mi></mml:msup></mml:mrow></mml:mfenced><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:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          with <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> the mean annual potential evaporation, <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> the mean annual evaporation, <inline-formula><mml:math id="M23" display="inline"><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> the mean
annual precipitation and <inline-formula><mml:math id="M24" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> a shape factor, assumed to represent catchment characteristics (e.g., vegetation, soils). This equation can be
reformulated by dividing the left-hand side and right-hand side by <inline-formula><mml:math id="M25" display="inline"><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula>, followed by dividing the nominator and denominator on the right-hand side by <inline-formula><mml:math id="M26" display="inline"><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> as well, leading to
            <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M27" display="block"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mfrac></mml:mstyle><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mfrac></mml:mstyle></mml:mfenced><mml:mi>n</mml:mi></mml:msup><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msup><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e784">In a similar way, Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>) can be expressed by the ratio of <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>/</mml:mo><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> as the dependent variable. First,
both sides of Eq. (<xref ref-type="disp-formula" rid="Ch1.E1"/>) are divided by <inline-formula><mml:math id="M29" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> again, followed by dividing the nominator and denominator on the
right-hand side by <inline-formula><mml:math id="M30" display="inline"><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> (see also Supplement S1):
            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M31" display="block"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:msup><mml:mfenced open="(" close=")"><mml:mrow><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mi>n</mml:mi></mml:msup><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:mfenced><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msup><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e922">These two formulations are often used interchangeably, and data can be plotted in figures based on Eqs. (<xref ref-type="disp-formula" rid="Ch1.E2"/>) or (<xref ref-type="disp-formula" rid="Ch1.E3"/>). We
will adopt here dryness index projection and wetness index projection throughout the paper for projections based on Eqs. (<xref ref-type="disp-formula" rid="Ch1.E2"/>)
and (<xref ref-type="disp-formula" rid="Ch1.E3"/>), respectively, to refer to these different ways of applying the Budyko framework.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Fitting the Budyko equations</title>
      <p id="d1e941">The exponent <inline-formula><mml:math id="M32" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> in Eqs. (<xref ref-type="disp-formula" rid="Ch1.E2"/>) and (<xref ref-type="disp-formula" rid="Ch1.E3"/>) was fit to data of multiple catchments with a least-squares fit based on the
Levenberg–Marquardt algorithm <xref ref-type="bibr" rid="bib1.bibx19" id="paren.41"><named-content content-type="pre">python scipy.optimize.curve_fit,
<uri>https://docs.scipy.org/doc/scipy/reference/generated/scipy.optimize.curve_fit.html</uri>, last access: 10 February 2022,
</named-content></xref>. Normally, this algorithm minimizes the sum of the squared residuals; i.e., it uses a linear least-squares loss
function. Afterwards, instead of using a linear least-squares loss function, other loss functions to minimize the residuals were used, in order to
obtain a robust fit. These loss functions <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> are summarized in Table <xref ref-type="table" rid="Ch1.T1"/>, and the final, resulting loss function is
defined as
            <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M34" display="block"><mml:mrow><mml:msup><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>′</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:msup><mml:mi>C</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>⋅</mml:mo><mml:mi mathvariant="italic">ρ</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:msup><mml:msub><mml:mi>x</mml:mi><mml:mi>r</mml:mi></mml:msub><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>/</mml:mo><mml:msup><mml:mi>C</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          with <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>r</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> the residual of data point <inline-formula><mml:math id="M36" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M37" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> a scale parameter, <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> the resulting loss and <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>(</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> the loss function (see
Table <xref ref-type="table" rid="Ch1.T1"/>). The scale parameter <inline-formula><mml:math id="M40" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> generally separates outliers from the data and was given different values between 0.1 and 1
in order to vary the data points that are considered as outliers, where low values of <inline-formula><mml:math id="M41" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> classify the most data points as outliers. Note that <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:mi>C</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>
with a linear loss function results in an ordinary least-squares fit again.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e1101">Loss functions used for fitting the Budyko curves, from <uri>https://docs.scipy.org/doc/scipy/reference/generated/scipy.optimize.curve_fit.html</uri>, last access: 10 February 2022.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Method</oasis:entry>
         <oasis:entry colname="col2">Equation</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Linear</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Soft</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2</mml:mn><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>z</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:msup><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Huber</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mfenced open="{" close=""><mml:mtable class="cases" columnspacing="1em" rowspacing="0.2ex" columnalign="left left" framespacing="0em"><mml:mtr><mml:mtd><mml:mrow><mml:mi>z</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext>if </mml:mtext><mml:mi>z</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>⋅</mml:mo><mml:msup><mml:mi>z</mml:mi><mml:mn mathvariant="normal">0.5</mml:mn></mml:msup><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mtext>otherwise</mml:mtext><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Cauchy</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>+</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Arctan</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mtext>arctan</mml:mtext><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>CAMELS data</title>
      <p id="d1e1347">In order to test the different hypotheses, the CAMELS data <xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx25" id="paren.42"/> were used, as they provide a large dataset
of 671 catchments across the contiguous United States. For each catchment in this dataset, daily discharge, rainfall, potential evaporation and air
temperature are available. Eventually, 357 catchments were selected based on several conditions similar to <xref ref-type="bibr" rid="bib1.bibx15" id="text.43"/>.
<list list-type="bullet"><list-item>
      <p id="d1e1358">positive long-term mean discharge: <inline-formula><mml:math id="M48" display="inline"><mml:mover accent="true"><mml:mi>Q</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> <inline-formula><mml:math id="M49" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 0 <inline-formula><mml:math id="M50" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></p></list-item><list-item>
      <p id="d1e1395">positive long-term mean precipitation: <inline-formula><mml:math id="M51" display="inline"><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> <inline-formula><mml:math id="M52" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 0 <inline-formula><mml:math id="M53" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">yr</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></p></list-item><list-item>
      <p id="d1e1432">runoff ratio smaller than unity: <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:mover accent="true"><mml:mi>Q</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>/</mml:mo><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M55" display="inline"><mml:mo>≤</mml:mo></mml:math></inline-formula> 1</p></list-item><list-item>
      <p id="d1e1461">long-term actual evaporation not exceeding potential evaporation: <inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mover accent="true"><mml:mi>Q</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>/</mml:mo><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M57" display="inline"><mml:mo>≤</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mrow></mml:math></inline-formula></p></list-item><list-item>
      <p id="d1e1514">no lakes: water fraction <inline-formula><mml:math id="M59" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 5 %</p></list-item><list-item>
      <p id="d1e1525">no snow-dominated catchments: mean elevation <inline-formula><mml:math id="M60" display="inline"><mml:mo>≤</mml:mo></mml:math></inline-formula> 2000 <inline-formula><mml:math id="M61" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> and snow days <inline-formula><mml:math id="M62" display="inline"><mml:mo>≤</mml:mo></mml:math></inline-formula> 20 %</p></list-item><list-item>
      <p id="d1e1551">relatively large catchments: area <inline-formula><mml:math id="M63" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 100 <inline-formula><mml:math id="M64" display="inline"><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">km</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>.</p></list-item></list></p>
      <p id="d1e1572">Afterwards, the actual evaporation was determined based on the long-term water balance, assuming that storage change is negligible over a longer period
of time:
            <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M65" display="block"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>-</mml:mo><mml:mover accent="true"><mml:mi>Q</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          with <inline-formula><mml:math id="M66" display="inline"><mml:mover accent="true"><mml:mi>P</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> the mean annual precipitation, <inline-formula><mml:math id="M67" display="inline"><mml:mover accent="true"><mml:mi>Q</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> the mean annual discharge and <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>E</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> the mean annual actual
evaporation. In this way, all water balance components are known to plot the data in the Budyko space.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Approach</title>
      <p id="d1e1648">The research question was addressed by a simple approach. First, the Budyko curves were fit to the CAMELS data with the different loss functions as
defined in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2"/>, in the two different projections. This was done for the selected 357 catchments all together, as well as for
catchments grouped by a high aridity (<inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, 247 catchments) and a low aridity (<inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, 110 catchments), the latter to
assess whether differences start to occur when catchments are dominantly in either the contracted side of the framework (i.e., <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>
or <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>≥</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>) or the non-contracted side of the framework. The vertical distances to the curve as well as the distances to the envelope
of the physical limits were calculated for the different projections.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e1731">CAMELS dataset plotted in different projections of the Budyko space, with <bold>(a)</bold> and <bold>(c)</bold> a projection normalized by precipitation for all catchments and <bold>(b)</bold>, and <bold>(d)</bold> a projection normalized by potential evaporation. In <bold>(c)</bold> and <bold>(d)</bold> the catchments are split into two groups that are either water-limited or energy-limited, with the best fit curve for all catchments in black, the best fit for the group of energy-limited catchments in red and the best fit for the group of water-limited catchments in blue. The differences between the curves in <bold>(c)</bold> and <bold>(d)</bold> are shown in <bold>(e)</bold> for a projection normalized by precipitation, whereas <bold>(f)</bold> shows the differences between the curves in <bold>(c)</bold> and <bold>(d)</bold> for a projection normalized by potential evaporation.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/4575/2022/hess-26-4575-2022-f01.png"/>

        </fig>

      <p id="d1e1778">In the next step, the uncertainty in the estimated mean annual actual evaporation due to the different projections was assessed. This was done by
selecting one catchment for the prediction of mean annual actual evaporation, whereas the remaining 356 catchments were used to fit the Budyko
curve. This was again carried out in a projection based on a wetness index and a dryness index. As both estimates can be considered equally likely,
the uncertainty was defined as the relative difference from the mean of the two estimates (i.e., the difference between the estimates equals 2 times
the uncertainty). In addition, the predictions were evaluated by the relative error compared with the water balance based observed evaporation. The
procedure was repeated for each catchment, leading to uncertainty estimates and relative errors for each catchment. Eventually, predictions were also
made by just using the non-contracted side of the framework.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e1784">Fitted <inline-formula><mml:math id="M73" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values for <bold>(a)</bold> all catchments, <bold>(b)</bold> energy-limited catchments and <bold>(c)</bold> water-limited catchments, for projections that normalized by precipitation (blue) and potential evaporation (red). On the <inline-formula><mml:math id="M74" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis, the different robust regression methods with different scale parameters (separating outliers from the data) are shown. </p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/4575/2022/hess-26-4575-2022-f02.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results and discussion</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Fitting the Budyko curve for different projections</title>
      <p id="d1e1832">Fitting the selected catchments of the CAMELS dataset to the two different projections led to different values for the <inline-formula><mml:math id="M75" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> exponent in
Eqs. (<xref ref-type="disp-formula" rid="Ch1.E2"/>) and (<xref ref-type="disp-formula" rid="Ch1.E3"/>) (Fig. <xref ref-type="fig" rid="Ch1.F1"/>a and b, <inline-formula><mml:math id="M76" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M77" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 2.254 and <inline-formula><mml:math id="M78" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M79" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 2.037, respectively). These
<inline-formula><mml:math id="M80" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values differed even stronger when the catchments were separated into two groups based on their aridity (<inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, respectively, Fig. <xref ref-type="fig" rid="Ch1.F1"/>c and d). In particular, for the energy-limited catchments (<inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, shown in red), the
values changed strongly from an <inline-formula><mml:math id="M84" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> value of 2.181 in the projection with a dryness index (Fig. <xref ref-type="fig" rid="Ch1.F1"/>c) to a value of 1.967 in the
projection with a wetness index (Fig. <xref ref-type="fig" rid="Ch1.F1"/>d). The differences that occurred when the curves with the two different <inline-formula><mml:math id="M85" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values from the
two different projections were used in the same projection and subtracted from each other (Fig. <xref ref-type="fig" rid="Ch1.F1"/>e and f) also show that
especially the curves based on energy-limited catchments strongly deviated (<inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, shown in red). In contrast, the curves obtained
for water-limited catchments (<inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, blue) remained more similar, with negligible differences.</p>
      <p id="d1e2003">The results presented in Fig. <xref ref-type="fig" rid="Ch1.F1"/> also strongly depended on the choice of the method, which was here a linear least-squares
fit. Repeating the analysis with more robust methods (see Table <xref ref-type="table" rid="Ch1.T1"/>) led to smaller differences between <inline-formula><mml:math id="M88" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values in the two
projections, even though differences were still present (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a). In particular, the scale parameter <inline-formula><mml:math id="M89" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> (Eq. <xref ref-type="disp-formula" rid="Ch1.E4"/>) that
identifies data points as outliers had a strong effect on the resulting <inline-formula><mml:math id="M90" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values when set to a larger value. Nevertheless, differences still occurred
for small values of this scale parameter, i.e the most stringent values that classify the most data points as outliers, even though these differences
became relatively minor. In contrast to what was found with the linear least-squares method, the robust methods resulted in differences in <inline-formula><mml:math id="M91" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values
for the water-limited catchments (Fig. <xref ref-type="fig" rid="Ch1.F2"/>c, differences between blue and red points) that are generally bigger than the
differences in <inline-formula><mml:math id="M92" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values for the energy-limited catchments (Fig. <xref ref-type="fig" rid="Ch1.F2"/>b, differences between blue and red points).</p>
      <p id="d1e2054">The above results clearly show that the projection used to fit the Budyko curve leads to different <inline-formula><mml:math id="M93" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values. Hence, <inline-formula><mml:math id="M94" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values that are found by
fitting Budyko-type curves include a rather high uncertainty, and the interpretation should be carried out with care. This does not necessarily lead
to large issues when <inline-formula><mml:math id="M95" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values are considered a characteristic for one single catchment <xref ref-type="bibr" rid="bib1.bibx49 bib1.bibx11 bib1.bibx35" id="paren.44"><named-content content-type="pre">e.g.,</named-content></xref>, as the equations can be solved analytically when just one data point is considered. However, the two formulations of the
curve (Eqs. <xref ref-type="disp-formula" rid="Ch1.E2"/> and <xref ref-type="disp-formula" rid="Ch1.E3"/>) stem from the same original equation (Eq. <xref ref-type="disp-formula" rid="Ch1.E1"/>), meaning that the definition and
value of the parameter should, in principle, not change when projections are changed. For this reason, the different values of the <inline-formula><mml:math id="M96" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> parameter found
here for the different projections express an additional uncertainty due to the choice of projection. When a Budyko curve is fit to multiple
catchments and the resulting <inline-formula><mml:math id="M97" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values are used for interpretation, this additional uncertainty should be considered.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Distances to the curve and envelopes</title>
      <p id="d1e2112">Once a Budyko curve is fit to the data, the distance to this curve is often used as a metric for catchment analysis
<xref ref-type="bibr" rid="bib1.bibx34 bib1.bibx48 bib1.bibx42" id="paren.45"><named-content content-type="pre">e.g.,</named-content></xref> and supposed to tell something about the state of the catchment,
catchment characteristics or the local climate. However, the distance to the curve strongly changed depending on the projection, and the differences
in distances depended on the aridity of the catchments (Fig. <xref ref-type="fig" rid="Ch1.F3"/>a). For energy-limited catchments (<inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>), the
distances to the curve were lower for the projection with a wetness index in comparison with the projection with a dryness index (i.e., catchments plot
left of the <inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> line in Fig. <xref ref-type="fig" rid="Ch1.F3"/>a), whereas the opposite was true for the water-limited catchments (right of the <inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> line in
Fig. <xref ref-type="fig" rid="Ch1.F3"/>a). This was also more generally confirmed when random samples in the Budyko space were used; see Supplement S2. The distances
to the physical boundaries are less often used as a metric for catchment analysis, but these changed similarly (Fig. <xref ref-type="fig" rid="Ch1.F3"/>b).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e2174">Vertical distances to <bold>(a)</bold> the envelope of the physical limits of the Budyko framework and <bold>(b)</bold> vertical distances to the fitted Budyko curve, both for projections normalized by precipitation (<inline-formula><mml:math id="M101" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axes) and potential evaporation (<inline-formula><mml:math id="M102" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axes). Water-limited catchments (<inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>) are shown by stars, whereas energy-limited catchments are shown by crosses. The color scale indicates the aridity of the catchments.</p></caption>
          <?xmltex \igopts{width=227.622047pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/4575/2022/hess-26-4575-2022-f03.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e2224">Uncertainty bounds of predicted values of <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, due to different projections <bold>(a)</bold>. The uncertainty is defined as the relative difference from the expected value of <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, which is the mean of the predicted values in the two different projections. The relative errors compared with observed (water balance) <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are shown in <bold>(b)</bold> for a dryness index projection (red), a wetness index projection (blue) and when only the non-contracted sides of the framework are used (gray). Note that for the blue and red boxplots, the full data are always used to derive the curve, whereas the gray boxplots only used the non-contracted side of the curve. For the gray boxplot with “All data”, the non-contracted sites were used as well; i.e., the curve was fit for catchments with <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> in a wetness index projection and for catchments with <inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> in a dryness index projection.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/4575/2022/hess-26-4575-2022-f04.png"/>

        </fig>

      <p id="d1e2312">These findings imply as well that exchanging projections of the Budyko curve is not as straightforward as it seems and may result in different
outcomes. Moreover, different interpretations can be given to these distances, as an increased distance to <inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:mi>E</mml:mi><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> indicates a decreased
energy use efficiency, whereas an increased distance to <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mi>E</mml:mi><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> indicates a decreased rain use efficiency by evaporation. In the literature, several
studies focus on explaining these distances to the curve <xref ref-type="bibr" rid="bib1.bibx10 bib1.bibx9 bib1.bibx43 bib1.bibx13" id="paren.46"><named-content content-type="pre">e.g., </named-content></xref>, rather than the <inline-formula><mml:math id="M111" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values, but usually only consider one specific projection. Thus, one needs to be aware that these
explanations are only valid for that specific projection because the meaning, as well as the value of these distances, changes for a different
projection.</p>
      <p id="d1e2362">Therefore, also here a consistent use of the framework is needed. As an aridity of 1.0 introduces a clear distinction between under- and
overestimating the distances to the curve and envelope in Fig. <xref ref-type="fig" rid="Ch1.F3"/>a and b, one may consider using only the side of the curve with
<inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula> in the dryness index projection or <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula> in the wetness index projection. In this way, the contracted side of
the curve is not used, which could lead to errors due to seemingly low absolute deviations that are in relative terms clearly present.</p><?xmltex \hack{\newpage}?>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Uncertainty in predictions</title>
      <p id="d1e2414">The Budyko framework is often used to predict values of <inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for ungauged catchments, but the uncertainty in predictions of <inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
due to the projection used exceeded 1.5 % for catchments with an aridity around 1.0 (Fig. <xref ref-type="fig" rid="Ch1.F4"/>a). In addition, the relative error
compared with the observed <inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> was especially large for energy-limited catchments of the CAMELS dataset (<inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>,
Fig. <xref ref-type="fig" rid="Ch1.F4"/>b). However, the differences in the relative errors between the dryness and wetness index based estimates remained rather
small (Fig. <xref ref-type="fig" rid="Ch1.F4"/>b).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e2478">Vertical distances to the envelope for a projection with a dryness index <bold>(a)</bold> and a wetness index <bold>(b)</bold>, with the same selection in catchments in blue triangles, red dots and black crosses. Distances to the envelope are shown in <bold>(c)</bold> as a function of the dryness index, with the distances to the non-contracted side in a projection with a dryness index in red (i.e., <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula> with distances <inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi></mml:mrow></mml:math></inline-formula>) and the distances to the non-contracted side in a projection with a wetness index in blue (i.e., <inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> with distances <inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>).</p></caption>
          <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://hess.copernicus.org/articles/26/4575/2022/hess-26-4575-2022-f05.png"/>

        </fig>

      <p id="d1e2576">The uncertainty in predicted values of <inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> due to the choice of projection in the Budyko framework has not received much attention to
date. Uncertainty evaluations do exist for the Budyko framework or derivatives thereof <xref ref-type="bibr" rid="bib1.bibx46" id="paren.47"><named-content content-type="pre">e.g.,</named-content></xref>, but these studies did not
consider the influence of different projections. Only <xref ref-type="bibr" rid="bib1.bibx2" id="text.48"/> noted that the chosen projection may lead to ambiguities,
especially related to leaky or gaining catchments. Implicitly, others may include the projection-related uncertainty indirectly by defining the curves
in a more statistical way <xref ref-type="bibr" rid="bib1.bibx16" id="paren.49"/>, but we would still argue that the influence of the projection used needs more consideration.</p>
</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Influence of outliers</title>
      <p id="d1e2609">An important cause of the different <inline-formula><mml:math id="M123" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values in the different projections are data points that appear as outliers in one projection but not in the
other projection. For example, several data points have short vertical distances to the envelope in a dryness index projection but have large
distances to the envelope in a wetness index projection and could be considered as outliers (red points in Fig. <xref ref-type="fig" rid="Ch1.F5"/>a and b). Vice
versa, one data point appears as an outlier in a dryness-index-based projection (blue point in Fig. <xref ref-type="fig" rid="Ch1.F5"/>a), but this is not apparent
in the other projection (Fig. <xref ref-type="fig" rid="Ch1.F5"/>b).</p>
      <p id="d1e2625">The outliers also influenced the relative errors when the curve was used to predict <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. The group of catchments identified as outliers in
a wetness index projection (i.e., red points in Fig. <xref ref-type="fig" rid="Ch1.F5"/>) led to lower <inline-formula><mml:math id="M125" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values with a lower curve (see also
Fig. <xref ref-type="fig" rid="Ch1.F1"/>) and a predicted <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> that is more often underestimated (blue boxes in Fig. <xref ref-type="fig" rid="Ch1.F4"/> shifted
downwards). Once only the non-contracted side of the framework was used for predictions, the relative errors became either more negative (for
<inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>) or improved and approached 0 (for <inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>). However, this was merely a result of the absence of the group of
outliers (with <inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>) for the predictions of the catchments with <inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>. Thus, using only the contracted sides of the
framework does not necessarily improve predictions of <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. Nevertheless, we would still argue that plotting the framework in the two
projections and, at least, inspecting the non-contracted sides for outliers is a valuable and necessary step in Budyko applications.</p>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Conclusions</title>
      <p id="d1e2760">The Budyko framework was applied to a selection of catchments across the contiguous United States, with two different ways to plot the framework. The
first projection used a wetness index, whereas the second projection used a dryness index. First, curves were fit with a standard linear least-squares
algorithm, followed by more robust methods afterwards. Distances of individual catchments to the curves and envelopes were determined, in order to
assess to effects of the different projections. In the next step, we assessed the uncertainty in predicted values of actual evaporation due to the
different projections.</p>
      <p id="d1e2763">In this way, we gained the following insights:
<list list-type="bullet"><list-item>
      <p id="d1e2768">The differences in <inline-formula><mml:math id="M132" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values due to the projection used were <inline-formula><mml:math id="M133" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> 0.2 for this dataset (Fig. <xref ref-type="fig" rid="Ch1.F1"/>).</p></list-item><list-item>
      <p id="d1e2788">Robust fitting algorithms reduced the differences in <inline-formula><mml:math id="M134" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> values in the different projections, but differences were still present
(Fig. <xref ref-type="fig" rid="Ch1.F2"/>).</p></list-item><list-item>
      <p id="d1e2801">The distances to the curve had a systematic dependence on the projection, with larger differences for the non-contracted side of the framework,
i.e., <inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> for the projection with a dryness index and <inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mi>P</mml:mi><mml:mo>/</mml:mo><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> for the projection with a wetness index
(Fig. <xref ref-type="fig" rid="Ch1.F3"/>).</p></list-item><list-item>
      <p id="d1e2845">The resulting uncertainty in predicted values of <inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, solely due to the projections used, could exceed 1.5 %
(Fig. <xref ref-type="fig" rid="Ch1.F4"/>).</p></list-item><list-item>
      <p id="d1e2862">Data points can appear as outliers in one projection but not in the other, causing differences in the fitting of the curves
(Fig. <xref ref-type="fig" rid="Ch1.F5"/>).</p></list-item></list></p>
      <p id="d1e2867">These findings show that the projection used needs to be considered carefully. Here, we would like to argue to assess always the non-contracted side
of the framework in the two projections. Catchments that seem close to the curve and the limits on the contracted side can easily appear as strong
outliers on the non-contracted side of the framework, as the absolute value of the relative errors changes on the <inline-formula><mml:math id="M138" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis on the contracted side
(i.e., a 10 % error in <inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi></mml:mrow></mml:math></inline-formula> for <inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> differs in absolute terms for <inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi mathvariant="normal">p</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula>). In contrast, this does not
happen when only the non-contracted side is considered. At least, it must be noted and considered that the projection used does lead to differences
and adds uncertainty to analyses where Budyko curves are fit to multiple catchments. Studies that use Budyko-type curves should therefore assess
whether their results are robust and remain unchanged when the projection is changed.</p><?xmltex \hack{\newpage}?>
</sec>

      
      </body>
    <back><notes notes-type="codedataavailability"><title>Code and data availability</title>

      <p id="d1e2936">The full analysis, including all scripts and data, is available on Renku (<uri>https://renkulab.io/projects/remko.nijzink/budyko</uri>, <xref ref-type="bibr" rid="bib1.bibx26" id="altparen.50"/>; <ext-link xlink:href="https://doi.org/10.5281/zenodo.7068888" ext-link-type="DOI">10.5281/zenodo.7068888</ext-link>, <xref ref-type="bibr" rid="bib1.bibx27" id="altparen.51"/>).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e2951">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/hess-26-4575-2022-supplement" xlink:title="zip">https://doi.org/10.5194/hess-26-4575-2022-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e2960">Analyses, preprocessing and post-processing of data were carried out by RCN. SJS and RCN contributed to the final text.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e2966">At least one of the (co-)authors is a member of the editorial board of <italic>Hydrology and Earth System Sciences</italic>. The peer-review process was guided by an independent editor, and the authors also have no other competing interests to declare.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e2975">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e2981">This study is part of the WAVE project, funded by the Luxembourg National Research Fund (FNR) ATTRACT programme (A16/SR/11254288). We thank NCAR for making the CAMELS data available (<uri>https://ral.ucar.edu/solutions/products/camels</uri>, last access: 9 February 2022).</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e2989">This research has been supported by the Fonds National de la Recherche Luxembourg (FNR) ATTRACT programme (grant no. A16/SR/11254288).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e2995">This paper was edited by Adriaan J. (Ryan) Teuling and reviewed by two anonymous referees.</p>
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