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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-22-5057-2018</article-id><title-group><article-title>Combined impacts of ENSO and MJO on the 2015 growing season drought on the
Canadian Prairies</article-title><alt-title>Combined impacts of ENSO and MJO</alt-title>
      </title-group><?xmltex \runningtitle{Combined impacts of ENSO and MJO}?><?xmltex \runningauthor{Z. Li et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Li</surname><given-names>Zhenhua</given-names></name>
          <email>zhenhua.li@usask.ca</email>
        <ext-link>https://orcid.org/0000-0003-0220-2696</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Li</surname><given-names>Yanping</given-names></name>
          <email>yanping.li@usask.ca</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Bonsal</surname><given-names>Barrie</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Manson</surname><given-names>Alan H.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Scaff</surname><given-names>Lucia</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Global Institute for Water Security, University of Saskatchewan, Saskatoon, Saskatchewan,   Canada</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Institute of Space and Atmospheric Studies, University of Saskatchewan, Saskatoon, Saskatchewan, Canada</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>National Hydrology Research Centre, Environment and Climate Change Canada, Saskatoon, Saskatchewan,  Canada</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Yanping Li (yanping.li@usask.ca) and   Zhenhua Li (zhenhua.li@usask.ca)</corresp></author-notes><pub-date><day>1</day><month>October</month><year>2018</year></pub-date>
      
      <volume>22</volume>
      <issue>10</issue>
      <fpage>5057</fpage><lpage>5067</lpage>
      <history>
        <date date-type="received"><day>7</day><month>February</month><year>2018</year></date>
           <date date-type="rev-request"><day>23</day><month>February</month><year>2018</year></date>
           <date date-type="rev-recd"><day>23</day><month>July</month><year>2018</year></date>
           <date date-type="accepted"><day>23</day><month>July</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/22/5057/2018/hess-22-5057-2018.html">This article is available from https://hess.copernicus.org/articles/22/5057/2018/hess-22-5057-2018.html</self-uri><self-uri xlink:href="https://hess.copernicus.org/articles/22/5057/2018/hess-22-5057-2018.pdf">The full text article is available as a PDF file from https://hess.copernicus.org/articles/22/5057/2018/hess-22-5057-2018.pdf</self-uri>
      <abstract>
    <p id="d1e132">Warm-season precipitation on the Canadian Prairies plays a crucial role in
agricultural production. This research investigates how the early summer 2015
drought across the Canadian Prairies is related to the tropical Pacific
forcing. The significant deficit of precipitation in May and June 2015
coincided with a warm phase of the El Niño–Southern Oscillation (ENSO) and a
negative phase of Madden–Julian Oscillation (MJO)-4 index, which favour a
positive geopotential height (GPH) anomaly in western Canada. Our further
investigation during the instrumental record (1979–2016) shows that
warm-season precipitation in the Canadian Prairies and the corresponding
atmospheric circulation anomalies over western Canada teleconnected with the
lower boundary conditions in the tropical western Pacific. Our results
indicate that MJO can play a crucial role in determining the summer
precipitation anomaly in the western Canadian Prairies when the equatorial
central Pacific is warmer than normal (NINO4 &gt; 0) and MJO is more
active. This teleconnection is due to the propagation of a stationary Rossby
wave that is generated in the MJO-4 index region. When the tropical
convection around MJO-4 index region (western tropical Pacific, centred over
140<inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) is more active than normal (NINO4 &gt; 0), Rossby
wave trains originate from the western Pacific with wavenumbers determined by
the background mean wind and meridional absolute vorticity gradient. Under
warm NINO4 conditions waves are generated with smaller wavenumbers compared
to cold NINO4 conditions. These waves under warm NINO4 can propagate into the
mid-latitudes over North America, causing a persistent anomalous ridge in the
upper level over western Canada, which favours dry conditions over the
region.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e151">The Canadian Prairies depend on summer precipitation especially during the
early to mid-growing season (May through August) when the majority of annual
precipitation normally occurs (e.g., Bonsal et al., 1993). High natural
variability in growing season precipitation causes periodic occurrences of
extreme precipitation (Li et al., 2017; Liu et al., 2016) and droughts that
are often associated with reduced agriculture yields, low streamflow, and
increased occurrence of forest fires (Wheaton et al., 2005; Bonsal and
Regier, 2007). Drought events with great environmental and economic impacts
on the Canadian Prairies have occurred in 1961, 1988, 2001–2002, and as
recent as 2015 (Dey, 1982; Liu et al., 2004; Bonsal et al., 1999; Wheaton et
al., 2005; Shabbar et al., 2011; Bonsal et al., 2013; Szeto et al., 2016).
The sub-seasonal forecast of precipitation for the growing season is crucial
for the agriculture, water resource management, and the economy of the
region. Therefore, an investigation into the causes of inter-annual
variability in the growing season precipitation of the Canadian Prairies is
needed.</p>
      <p id="d1e154">Low precipitation and extended dry periods on the Canadian Prairies are
often associated with an upper-level ridge and a persistent high pressure
centred over the region (Dey, 1982; Liu et al., 2004). These prolonged atmospheric
anomalies often concurred with abnormal boundary layer conditions such as a
large-scale sea surface temperature (SST) anomalies in the Pacific Ocean
(Shabbar and Skinner, 2004). Large-scale oscillation in the SST anomalies in
the Pacific Ocean, namely El Niño and the Pacific Decadal Oscillation
(PDO), can affect the hydroclimatic pattern in summer over North America,
although the strongest impacts of<?pagebreak page5058?> these boundary conditions occur during the
boreal winter. Inter-annual variability such as El Niño–Southern Oscillation
(ENSO) is linked with extended droughts in the Prairies (Bonsal et al., 1999;
Shabbar and Skinner, 2004). Interdecadal oscillations such as the PDO and
the Atlantic Multi-decadal Oscillation (AMO) also affect the seasonal
temperature and precipitation in the Canadian Prairies (Shabbar et al., 2011).</p>
      <p id="d1e157">ENSO's relationship with the Canadian Prairies' precipitation has been
studied extensively. Previous investigations (e.g., Shabbar et al., 2011)
have found that El Niño events are associated with a summer moisture
deficit in western Canada while La Niña events cause an abundance of
moisture in far western Canada (British Columbia and Yukon). However, they
also noted that, although tropical SST variability accounted for some aspects
of the large-scale circulation anomalies that influence the Canadian Prairies
meteorological drought, a consistent and clear-cut relationship was not
found. The warm phase of ENSO often favours drought in this region,
especially during the growing season after the mature phase of El Niño
(Bonsal and Lawford, 1999; Shabbar and Skinner, 2004). The positive North
Pacific Mode
(NPM, Hartmann et al., 2015) like the North Pacific SST anomaly pattern often
follows a matured El Niño, and the accompanying atmospheric ridging leads
to extended dry spells over the Prairies during the growing season (Bonsal
and Lawford, 1999). Furthermore, in association with the recent North Pacific
SST anomaly from 2013 to 2014, researchers have attributed the precipitation
deficit in California during 2013 to the anomalous upper-level ridge over
western North America (Wang et al., 2014; Szeto et al., 2016).</p>
      <p id="d1e160">The aforementioned SST variations mostly vary on inter-annual and decadal
scales. Another important factor that affects the weather patterns in North
America is the Madden–Julian Oscillation (MJO), an intra-seasonal
(40–90 days) oscillation in convection and precipitation pattern over the
tropics (Madden and Julian, 1971; Zhang, 2005; Riddle et al., 2013; Carbone
and Li, 2015). MJO is a coupled atmosphere–ocean oscillation involving
convection and large-scale equatorial waves, which produces an eastward
propagation of the tropical convection anomaly (Madden and Julian, 1971). The
MJO affects the winter temperature and precipitation in North America and
Europe through its impact on moisture transport associated with the
“Pineapple Express” and its effects on the North Atlantic Oscillation and
stratospheric polar vortex (Cassou, 2008; Garfinkel et al., 2012; Rodney et
al., 2013). MJO is also connected to the summer precipitation anomalies in
the southwestern United States (Lorenz and Hartmann, 2006). During the warm
season, MJO's impact on the Canadian Prairies' precipitation has not been
thoroughly investigated as MJO's amplitude is weak during spring and early
summer. The amplitude of MJO in spring and early summer is related to the
inter-annual variation of the tropical SST, especially the SST in the central
Pacific (Hendon et al., 2007; Marshall et al., 2016). MJO in terms of the
Real-time Multivariate MJO index (RMM, Wheeler and Hendon, 2004) was
extremely strong in the early spring of 2015 with a positive PDO-like SST
anomaly in the central Pacific and, at the same time, El Niño started to
strengthen.</p>
      <p id="d1e164">MJO activities in the western Pacific under the modulation of inter-annual
SST variability have the potential to act together with ENSO and impact
mid-tropospheric circulation over western Canada and, thus, warm-season
precipitation over the Canadian Prairies. The goal of this study is to
demonstrate that MJO has contributed to the 2015 growing season drought in
the Canadian Prairies through the propagation of stationary Rossby waves.
Subsequently, further investigations are carried out to determine if similar
relationships exist in association with other summer extreme precipitation
events during the instrumental record (1979–2016). Section 2 provides the
datasets and methodology used in this paper while Sect. 3 presents the
analysis of the upper-level circulation anomaly and SST pattern associated
with the 2015 drought. This is followed by the examination of the effects of
central Pacific SST anomalies and MJO on the summer precipitation in the
Canadian Prairies. The mechanism by which MJO affects summer precipitation
when equatorial central Pacific SST is warmer than normal is discussed in
Sect. 4, followed by the summary and concluding remarks in Sect. 5.</p>
</sec>
<sec id="Ch1.S2">
  <title>Data and methodology</title>
      <p id="d1e173">Multiple observation and reanalysis datasets are used to investigate the
circulation anomalies associated with the Canadian Prairies' growing season
(May–August) precipitation. The observed precipitation is taken from the
Climate Prediction Center (CPC) Merged Analysis of Precipitation (CMAP)
dataset (Xie and Arkin, 1997; NOAA CPC, 2017a). Geopotential height (GPH)
fields from the National Centers for Environmental Predictions (NCEP)
Reanalysis (Kalnay et al., 1996; NOAA NCEP, 2017) and the European Centre for
Medium-Range Weather Forecast's (ECMWF) ERA-Interim reanalysis (Dee et al.,
2011; ECMWF, 2017) are used to analyze the mid- and upper-level (500 and
200 hPa) atmospheric circulation patterns.</p>
      <p id="d1e176">To represent the central Pacific SST anomaly, the NINO4 SST index (Rayner et
al., 2003; NOAA, 2017b) from the CPC of the National Oceanic and Atmospheric
Administration (NOAA) is used since the NINO4 region is near the central
Pacific and spans over the dateline (5<inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S–5<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N,
160<inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E–150<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W). Multivariate ENSO Index (NOAA, 2017c) data
are retrieved from NOAA's Climate Data Center (CDC) website and are used to
determine the ENSO phase (Wolter, 1987; Wolter and Timlin, 1993). In
particular, the El Niño condition is defined when the monthly mean index
of MEI is larger than 0.5 (Andrews et al., 2004).</p>
      <p id="d1e215">The Real-time Multivariate MJO series (RMM1 and RMM2; Bureau of Meteorology
of Australia, 2017) developed by Wheeler and Hendon (2004) are used to
identify<?pagebreak page5059?> periods of strong MJO activity as the MJO amplitudes are directly
calculated by the square root of RMM1 <inline-formula><mml:math id="M6" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> RMM2. For MJO intensities over
the investigated regions, we used the monthly averaged pentad MJO indices
from the NOAA CPC's MJO index (Xue et al., 2002; NOAA CPC, 2017b), which have
10 indices representing locations around the globe. The CPC's MJO index is
based on extended empirical orthogonal function (EEOF) analysis on pentad
velocity potential at 200 hPa. A total of 10 MJO indices on a daily scale
are constructed by projecting the daily (00:00 UTC) velocity potential
anomalies at 200 hPa (CHI200) onto the 10 time-lagged patterns of the first
EEOF of pentad CHI200 anomalies (Xue et al., 2002). Negative values of 10 MJO
indices correspond to enhanced convection in the 10 regions centred on
20<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, 70<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, 80<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, 100<inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E,
120<inline-formula><mml:math id="M11" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, 140<inline-formula><mml:math id="M12" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, 160<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, 120<inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W,
40<inline-formula><mml:math id="M15" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W, and 10<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W in the tropics. MJO indices usually vary
between <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> and 2, with negative values indicating above-average convective
activities in the corresponding region. Because boreal summer usually
corresponds to a period of a weaker amplitude of MJO than the winter, we
chose the monthly mean value of <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula> as the criterion of strong convection
which is connected to MJO as the indices generally vary between <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> and 1.
An MJO-4 index (centred on 140<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) of less than <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula> was
considered a relatively strong convection in the western Pacific, which has
been found to be a source region of stationary Rossby waves (Simmons and
Hoskins, 1980). SST observations include the Extended Reconstructed Sea
Surface Temperature (ERSST) v4 (NOAA, 2017a; Huang et al., 2015). Outgoing
Longwave Radiation (NOAA, 2017d) data from NOAA Interpolated Outgoing
Longwave Radiation are used to derive the composite of anomalies of OLR for a
certain phase of MJO.</p>
      <p id="d1e366">Our study focuses on the growing season precipitation in the provinces of
Alberta and Saskatchewan in the Canadian Prairies, where the largest
deficits were observed in 2015. Specifically, the regional mean
precipitation over 115–102.5<inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W, 50–57.5<inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N is used
(boxed area in Fig. 1, top panel) to represent
the Canadian Prairies east of the Rocky Mountains and south of the boreal
forest. The chosen region also covers most of the arable land in the
Canadian Prairies. Considering the unique MJO-4 and NINO4 indices for 2015,
the relationship between the Prairies' warm-season (May–August)
precipitation with MJO-4 and ENSO during the instrumental records is
investigated using correlation and regression. Though the dry months of the
2015 growing season are May and June when MJO-4 was in negative phase, we
want to study the statistical relationship between MJO-4 and the Prairies'
precipitation in the whole period of the growing season (May–August). The
possible mechanism behind the correlation between MJO-4 and the Prairies'
warm-season precipitation under El Niño condition is further investigated by
analyzing the upper-level circulation associated with convection in the
tropical Pacific and stationary Rossby waves in mid-latitudes.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p id="d1e390"><bold>(a)</bold> Precipitation anomalies (mm) from CMAP over the region
(115–102.5<inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W,
50–57.5<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N) during May and June 2015. <bold>(b)</bold> Time series of
monthly precipitation anomaly over the boxed region (shown in <bold>a</bold>) between September 2013 and
August 2015.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/5057/2018/hess-22-5057-2018-f01.png"/>

      </fig>

</sec>
<sec id="Ch1.S3">
  <title>Results</title>
<sec id="Ch1.S3.SS1">
  <title>The 2015 summer drought</title>
      <p id="d1e436">Almost all of western Canada including British Columbia, the southern
Northwest Territories, Alberta, and Saskatchewan had negative precipitation
anomalies during May and June 2015. The top plot in Fig. 1 shows the
precipitation anomaly in percentage relative to the climatology (1981–2010
long-term mean) in Canada during May and June 2015. The bottom plot in Fig. 1
presents the monthly precipitation anomaly averaged over the region
encompassed by the dashed lines (top panel in Fig. 1). The average annual cycle
of the regional precipitation has a dry period between February and May and
June has the largest precipitation in all months. The May and June 2015
precipitation deficit was also accompanied by a relatively dry period from
February to April (Fig. 1 and Szeto et al., 2016), which added to the drought
conditions.</p>
      <p id="d1e439">The 500 hPa geopotential height anomaly averaged in May and June is
examined together with the SST anomaly and ENSO, as well as MJO-4 indices for 2014 and
2015. The 500 hPa GPH anomaly for May and June 2015 shows strong positive
anomalies near Alaska and the British Columbia coast (Fig. 2), which is
consistent with the findings for other episodes of growing season droughts
(e.g., Dey, 1982; Bonsal and Wheaton, 2005). Accompanying this anomalous
ridge are above-normal SSTs in the northeast Pacific off<?pagebreak page5060?> the coast of North
America and the central-eastern Pacific (Fig. 3). Both ENSO and the NPM are
in positive phases that correspond to a warmer SST near the Pacific coast of
North America, consistent with the positive GPH anomalies in western Canada
and Alaska. The ridge in Alaska/Bering Strait and the one near the British
Columbia coast have been previously associated with El Niño and the North
Pacific SST anomaly such as NPM (Shabbar et al., 2011). The monthly mean anomalous
ridge prevents storms from reaching the British Columbia coast and the
Canadian Prairies, causing extended dry spells. Therefore, the GPH anomaly in
the early growing season in 2015 is consistent with the precipitation anomaly in
these regions. The anomalous upper-level ridge in the western United States
and Canada in 2014 and 2015 has also been associated with the developing El Niño and the other main components of Pacific SST variation such as NPM by
several recent studies (Hartmann et al., 2015; Lee et al., 2015; Li et al., 2017).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><caption><p id="d1e444">NCEP GPH anomaly at 500 hPa during May and June 2015 when the
precipitation deficit was the largest.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/5057/2018/hess-22-5057-2018-f02.png"/>

        </fig>

      <p id="d1e453">The SST anomaly and the associated oscillations and modes, especially ENSO,
show consistent agreement with the observed GPH anomaly pattern. The average
SST anomaly during the growing season (May–June, July–August) of 2015 shows
a persistent strong positive anomaly in the northeast and eastern equatorial
Pacific (Fig. 3), which corresponds to the warm phase of NPM and ENSO. SSTs
in the eastern tropical Pacific warmed increasingly since the end of 2014 and
qualified as an El Niño in early 2015. The NPM became positive in fall
2013, turned exceptionally strong in 2014, and persisted to 2015 (Hartmann,
2015). The anomalous ridge is concurrent with strong SST anomalies in the
tropical Pacific and extratropical North Pacific. NPM, as the third
EOF of
Pacific SST (30<inline-formula><mml:math id="M26" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S–65<inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N), has also a strong connection to
the anomalous ridge in western North America and trough in the eastern US and
Canada in the 2013–2014 winter (Hartmann, 2015; Lee et al., 2015). During
the ENSO-neutral condition in 2013 and 2014, the precursor of ENSO, the
so-called “footprinting” mechanism is considered to cause this anomalous
ridge in western North America (Wang et al., 2014).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p id="d1e477">The mean SST anomaly (<inline-formula><mml:math id="M28" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C) from ERSST v4 for
May–June and July–August 2015.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/5057/2018/hess-22-5057-2018-f03.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p id="d1e497">RMM amplitude anomaly, NINO4, MJO-4 indices, and precipitation
anomaly of the Canadian Prairies from January 2014 to December 2015.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/5057/2018/hess-22-5057-2018-f04.png"/>

        </fig>

      <?pagebreak page5061?><p id="d1e506">The variation of the Canadian Prairies' precipitation and its relationship
with NINO4 and MJOs are shown in Fig. 4. The time series of the monthly RMM
amplitude, NINO4 index, MJO-4 indices, and the Canadian Prairies'
precipitation anomaly from January 2014 to December 2015 shows the
atmospheric–oceanic circulation indices for the drought in 2015. In May and
June 2015, the western Pacific witnessed a strong MJO-4 negative index,
whereas in July the MJO-4 index became positive. This corresponds well with
the precipitation anomaly in Fig. 1. As shown in Fig. 3, El Niño continued
to strengthen in July and August 2015, while at the same time the MJO-4
index increased. The increase in the MJO-4 index indicated that the active
convection associated with MJO moved away from the tropical western Pacific
region and propagated eastward into the central Pacific. Coincident with
this change in MJO, the precipitation in the Canadian Prairies then returned
to slightly above normal in July.</p>
      <p id="d1e509">The good correspondence of MJO-4 and the negative precipitation anomaly
suggests a link between MJO and Prairies precipitation during the growing
season. Although El Niño and the associated northeast Pacific SST warm anomaly
(i.e., NPM) in summer 2015 can be a contributing factor for the persistent
upper-level ridge over the west coast of Canada (Shabbar et al., 2011), it cannot
fully explain the drought condition in western Canada, as these SSTs do not
guarantee a prolonged dry spell as shown by correlation analysis (Table 1).
The negative MJO-4 index concurred with the negative anomaly of the
Prairies' growing season precipitation in 2015, which prompts the
investigation of their relationship with the instrumental records.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1"><caption><p id="d1e515">Correlation between mean precipitation anomaly in the Prairies from
CMAP and MEI, as well as MJO-4
indices. MJO indices
and CMAP are from 1979 to 2016.</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="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Correlation</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M29" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value</oasis:entry>
         <oasis:entry colname="col4">No. of</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">sample</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">MEI</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.096</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">0.24</oasis:entry>
         <oasis:entry colname="col4">156</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MJO-4</oasis:entry>
         <oasis:entry colname="col2">0.18</oasis:entry>
         <oasis:entry colname="col3">0.023</oasis:entry>
         <oasis:entry colname="col4">156</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MJO-4(NINO4 &gt; 0)</oasis:entry>
         <oasis:entry colname="col2">0.33</oasis:entry>
         <oasis:entry colname="col3">0.0015</oasis:entry>
         <oasis:entry colname="col4">90</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">MJO-4(NINO4 &lt; 0)</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">0.94</oasis:entry>
         <oasis:entry colname="col4">66</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><caption><p id="d1e649">The scatter plot of the monthly precipitation anomaly (mm month<inline-formula><mml:math id="M32" 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>)
as a function of MJO-4 and NINO4. Each asterisk represents a month from May
to August 1979–2016. Circled asterisks denote a month with precipitation
anomaly larger than 18 mm month<inline-formula><mml:math id="M33" 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 blue circles are months with
positive precipitation anomaly and the red circles are months with negative
precipitation anomaly. The sizes of circles denote the magnitudes of the
anomalies (large &gt; 30 mm month<inline-formula><mml:math id="M34" 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>,
medium &gt; 24 mm month<inline-formula><mml:math id="M35" 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>,
small &gt; 18 mm month<inline-formula><mml:math id="M36" 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 shaded area denotes
NINO4 &gt; 0 and MJO-4 index &lt; 0.</p></caption>
          <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/5057/2018/hess-22-5057-2018-f05.png"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS2">
  <title>Instrumental record</title>
      <p id="d1e724">El Niño and its associated North Pacific SST anomaly may contribute to
extended dry spells in Canadian Prairies after the mature phase of El Niño
(Bonsal et al., 1993) on an inter-annual timescale. ENSO, however, is not a
strong intra-seasonal-to-seasonal predictor of Canadian Prairies summer
precipitation. The lack of a strong correlation between the Prairies'
precipitation and ENSO index can be caused by the fact that many factors can
affect the Prairies' precipitation on a seasonal and sub-seasonal scale.
Shabbar and Skinner (2004) showed the connection between the warm phase of
ENSO and western Canadian drought through singular value decomposition
analysis. However, they also found other modes of SST variation (e.g., the
positive phase of PDO) can produce a wet condition in the Prairies. Here we
present a new result showing that, under warm central Pacific SST conditions
(NINO4 &gt; 0), a certain phase of MJO, which connected to the
active convection in the tropical western Pacific (Li and Carbone, 2012),
plays an important role in modulating the growing season precipitation in
the Canadian Prairies.</p>
      <p id="d1e727">The correlation coefficients between the mean regional precipitation anomaly
over Canadian Prairies and MJO-4 indices and MEI from May to August are
shown in Table 1. The correlation between MEI alone and the precipitation
anomalies is not significant. The correlation between MJO-4 and
precipitation in the Prairies is 0.18 with a <inline-formula><mml:math id="M37" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value of 0.023, which
indicates that stronger tropical convection in the equatorial region centred
around 140<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E favours less precipitation in the Canadian
Prairies from May to August. When NINO4 is larger than 0, the correlation
between MJO-4 and the growing season precipitation is 0.33 with a <inline-formula><mml:math id="M39" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value of
0.0015. Conversely, the correlation between MJO-4 and Canadian Prairies
precipitation is <inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula> when NINO4 &lt; 0.</p>
      <p id="d1e763">The scatter plot in Fig. 5 shows the distribution of monthly precipitation
anomaly versus the MJO-4 index and NINO4 index. Circled asterisks denote a
month with a precipitation anomaly larger than 18 mm month<inline-formula><mml:math id="M41" 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
red (blue) circles denote a negative (positive) precipitation anomaly. The
criterion for precipitation anomaly to be emphasized by the circles is
roughly one-third of the mean monthly precipitation in the growing season.
The size of the circle<?pagebreak page5062?> represents the magnitude of the monthly precipitation
anomalies with 6 mm month<inline-formula><mml:math id="M42" 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> interval. The bottom-right quadrant,
indicated by shading, shows that negative MJO-4 corresponds to many more dry
months than wet months under NINO4 &gt; 0 conditions. We noticed
that some significant dry months are not in the shaded area, which
corresponds to the dry months occurring during La Niña or in the period
after the mature phase of El Niño (Bonsal et al., 1999). Summer drought
in the Prairies can occur in both phases of ENSO or any other teleconnection
indices. For example, for the summer drought that happened in the Prairies
from 1999 to 2005, the large-scale anomalous patterns of SST first showed La
Niña conditions and then became a weak El Niño in the latter half of
the period (Hanesiak et al., 2011). Bonsal and Wheaton (2005) showed that the
tropospheric atmospheric circulation patterns in 2001 and 2002 lacked the
typical meridional flow in the North Pacific and North America during the
drought in western Canada. Their results show that the drought in 1999–2005
was related to the expansion of the continuous drought that happened in the
US to the north.</p>
      <p id="d1e790">The impact of ENSO on the growing season precipitation over the Canadian
Prairies is investigated through Fig. 6. The box-percentile plot in Fig. 6
shows the distribution of monthly Canadian Prairies' precipitation anomalies
from May to August along with different ENSO conditions. In general, under
El Niño and neutral ENSO conditions, the precipitation anomalies are centred
around 0, and there is no bias toward either end. Under La Niña condition,
the mean precipitation has a positive bias. There are only 10 summer months
under La Niña condition, whereas there are 71 months under El Niño and
neutral conditions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><caption><p id="d1e796">The box-percentile plot of the Canadian Prairies precipitation
anomaly during growing season under different ENSO conditions.</p></caption>
          <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/5057/2018/hess-22-5057-2018-f06.png"/>

        </fig>

      <p id="d1e805">The distributions of precipitation anomalies versus the MJO-4 index under
different ENSO conditions are shown in Fig. 7. For NINO4 &gt; 0, the
precipitation anomaly has a negative tendency when MJO-4 &lt; <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>.
With NINO4 &lt; 0, there is no negative tendency for MJO-4 &lt; <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.3</mml:mn></mml:mrow></mml:math></inline-formula>.
Therefore, Figs. 6 and 7 agree with the significant correlation
between precipitation and MJO-4 under NINO4 &gt; 0, relative to ENSO
in Table 1.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p id="d1e830">Box-percentile plots of the Canadian Prairies' precipitation anomaly
during growing season versus MJO-4 under warm NINO4 (NINO4 &gt; 0,
<bold>a</bold>) and cold NINO4 (NINO4 &lt; 0, <bold>b</bold>) SST
condition.</p></caption>
          <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/5057/2018/hess-22-5057-2018-f07.png"/>

        </fig>

      <p id="d1e845">The correlation between MJO-4 and the Prairies' precipitation during the
growing season leads us to investigate the underlying circulation anomalies.
Figure 8 presents the regressed stream function and wind field at 200 hPa in
the mid-latitudes (north of 30<inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N) on the negative MJO-4 index from
May to August under warm NINO4 SST condition (NINO4 &gt; 0.5). In
the tropics (10<inline-formula><mml:math id="M46" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S–20<inline-formula><mml:math id="M47" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N), during the Northern Hemisphere
summer, the OLR, velocity potential, and divergent wind vector are presented.
Only regression patterns having <inline-formula><mml:math id="M48" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> values lower than 0.05 are plotted for
OLR and velocity potential. The negative MJO-4 index corresponds to a
negative anomaly in OLR, stronger convection, and larger-than-average
divergence at 200 hPa in the region centre around 150<inline-formula><mml:math id="M49" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. The
strong convection anomaly centres around 150<inline-formula><mml:math id="M50" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, 5<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N with
divergent wind extending well<?pagebreak page5063?> into the subtropics in the Northern Hemisphere.
The positive GPH or stream
function anomaly extended from Japan to the central Pacific is associated
with the enhanced convection and divergence in the upper troposphere over the
western tropical–subtropical Pacific. A Rossby wave train linked to the OLR
anomaly and strong divergence in the western Pacific propagate eastward into
North America in the extratropics. To better demonstrate the propagation of
the wave train, we conducted a ray-tracing experiment of stationary Rossby
wave following the non-divergent barotropic Rossby wave theory of Hoskins and
Karoly (1981) and Hoskins and Ambrizzi (1993). Equation (1) describes the
group velocity, which represents the propagation of wave activity.
<inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">gx</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">gy</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the group velocity components on
zonal and meridional directions; <inline-formula><mml:math id="M54" display="inline"><mml:mover accent="true"><mml:mi>U</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> and <inline-formula><mml:math id="M55" display="inline"><mml:mover accent="true"><mml:mi>V</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula> are the
mean zonal and meridional winds; <inline-formula><mml:math id="M56" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> is the mean absolute vorticity; <inline-formula><mml:math id="M57" display="inline"><mml:mi>K</mml:mi></mml:math></inline-formula>,
<inline-formula><mml:math id="M58" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M59" display="inline"><mml:mi>l</mml:mi></mml:math></inline-formula> are the total wave number, zonal wavenumber, and meridional
wavenumber, respectively. The ray path is integrated using a fourth-order
Runge–Kutta method.

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M60" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">gx</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mover accent="true"><mml:mi>U</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>(</mml:mo><mml:msup><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>-</mml:mo><mml:msup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>)</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi>k</mml:mi><mml:mi>l</mml:mi><mml:msub><mml:mi>q</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msup><mml:mi>K</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E1"><mml:mtd/><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>C</mml:mi><mml:mi mathvariant="normal">gy</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mover accent="true"><mml:mi>V</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>(</mml:mo><mml:msup><mml:mi>k</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>-</mml:mo><mml:msup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>)</mml:mo><mml:msub><mml:mi>q</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi>k</mml:mi><mml:mi>l</mml:mi><mml:msub><mml:mi>q</mml:mi><mml:mi>y</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msup><mml:mi>K</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula></p>
      <p id="d1e1113">Under the average conditions in May–August derived from ERA-Interim at 200
hPa with NINO4 &gt; 0.5 or NINO4 &lt; <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula>, we released
rays with a total wavenumber matching with the mean flow at the extratropical
location of the OLR anomaly (140–150<inline-formula><mml:math id="M62" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, 25–30<inline-formula><mml:math id="M63" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N). For
quasi-stationary waves, the wavenumber is determined by the basic zonal flow
and background absolute vorticity gradient through the Rossby wave dispersion
relation. For the NINO4 &gt; 0.5 May–August condition, K <inline-formula><mml:math id="M64" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 4.14.
With this total wavenumber and launching angle from 0 to 60<inline-formula><mml:math id="M65" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> relative
to the zonal direction, Rossby wave rays (coloured by red, orange to blue
according to their angle from 0 to 60<inline-formula><mml:math id="M66" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>) released at 140<inline-formula><mml:math id="M67" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W,
20<inline-formula><mml:math id="M68" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N can propagate successfully to western Canada for those
with smaller launching angles (&lt; 30 <inline-formula><mml:math id="M69" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>) as shown in the bottom
plot in Fig. 9. With NINO4 &lt; <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula>, the zonal wind in the source
region is weaker, and the meridional gradient of absolute vorticity is
stronger due to its southern position relative to the subtropical
jet. The total wavenumber for stationary Rossby waves is 6.2, determined by
the mean May–August condition for NINO4 &lt; <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula>. The waves with
shorter wavelength tend to be evanescent near the source region as shown in
the top plot in Fig. 9. However, there is no significant difference in
ray path under the NINO4 &lt; <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> condition compared to
NINO4 &gt; 0.5 if the source wavenumbers are set to the same value
(results not shown). The changes in the mean conditions in the mid-latitudes
away from the source region from El Niño to La Niña are not sufficient to
alter the propagation condition for quasi-stationary Rossby waves.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><caption><p id="d1e1231">The regression of stream function and wind field in the extratropics on
negative MJO-4 for May–August with NINO4 &gt; 0.5 condition. In
the tropics, the regression of OLR, velocity potential, and divergent wind on
negative MJO-4 indices for May–August with NINO4 &gt; 0.5
condition. The shaded region for the tropical OLR has
<inline-formula><mml:math id="M73" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula> value &lt; 0.05. Blue shading indicates active convection region.
Red dashed contour and solid blue contour corresponds to negative and
positive velocity potential, respectively.</p></caption>
          <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/5057/2018/hess-22-5057-2018-f08.jpg"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9"><caption><p id="d1e1249">Ray-tracing result with total wavenumber specified by the mean flow
140–150<inline-formula><mml:math id="M74" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W and 20–30<inline-formula><mml:math id="M75" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N for mean May–August condition
with NINO4 &lt; <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> <bold>(a)</bold> and
NINO4 &gt; 0.5 <bold>(b)</bold>. Rays originate from 140<inline-formula><mml:math id="M77" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E,
20<inline-formula><mml:math id="M78" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, with angles ranging from 0 (red) to 60<inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> (dark blue)
from zonal direction.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://hess.copernicus.org/articles/22/5057/2018/hess-22-5057-2018-f09.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4">
  <title>Discussion</title>
      <p id="d1e1327">The summer of 2015 is the first summer after the development of El Niño during
the 2014–2015 winter. Though the upper-level GPH pattern, seen in summer 2015,
can be attributed to the SST modes in the Pacific, namely ENSO and NPM, the
precipitation in the western Canadian Prairies is not strongly correlated
with either. Bonsal and Lawford (1999) found that more extended dry spells
tend to occur in the Canadian Prairies during the second summer following
the mature stage of the El Niño events. The winter precipitation in Canada
has a strong connection to ENSO (Shabbar et al., 1997), whereas summer
precipitation, in most regions of western Canada (except the coast of
British Columbia and Southern Alberta), does not have a significant
correlation with ENSO. This is consistent with our investigation using
instrumental records from 1948 to 2016.</p>
      <p id="d1e1330">Growing season precipitation in the Canadian Prairies is affected by many
factors. Precipitation deficits can occur under various circulation and
lower boundary conditions. Thus, it is not expected that a universal
condition for all the significant droughts in the region can be identified.
In fact, extreme drought events have been found in both El Niño and La Niña
years. A previous study by Bonsal and Lawford (1999) indicates the
meteorological drought often occurs after the mature phase of El Niño, which
is not the case for 2015. The associated anomaly in the North Pacific
represented by the NPM positive phase is consistent with their results. The
direct linkage between ENSO and the summer precipitation in the Canadian
Prairies is not clear. In fact, the correlation between MEI and the
precipitation in the investigated region is <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.096</mml:mn></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.239</mml:mn></mml:mrow></mml:math></inline-formula>, sample
size <inline-formula><mml:math id="M82" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 152). The investigated region's growing season precipitation does not
possess a significant correlation with ENSO, which is consistent with other
researchers' findings (Dai and Wigley, 2000).</p>
      <p id="d1e1362">The regression pattern is consistent with stationary Rossby wave theory as
shown in a hierarchy of theoretical and modelling studies (Karoly et al.,
1989; Simmons et al., 1983; Hoskins and Ambrizzi, 1993; Ambrizzi and Hoskins,
1997; Held et al., 2002). A similar wave train extends from the western
Pacific toward extratropical South America but at lower latitudes compared to
its counterpart in the Northern Hemisphere (not shown). The node of the wave
train in western Canada and the
Pacific
Northwest of the US corresponds to an anomalous ridge, which is in phase
of El Niño forcing. When the convection in the region associated with
MJO-4 is weaker than normal (MJO-4 &gt; 0), a wave train with the
opposite sign will reach western Canada, which then counteracts the El
Niño forcing. Thus, the weak correlation between Canadian Prairies
precipitation and ENSO is understandable<?pagebreak page5064?> as MJO plays an additional role that
enhances or cancels out the GPH anomaly caused by El Niño.</p>
      <p id="d1e1365"><?xmltex \hack{\newpage}?>In the mid-latitude North America, the atmospheric response to the tropical
forcing in the western Pacific depends on the mean circulation condition
associated with tropical SST. Intraseasonal tropical convection oscillation
in the western Pacific associated with the MJO-4 index cannot determine the
sign of the precipitation anomaly in the Prairies alone. Both warm SST in the
central Pacific and strong tropical convection in the western Pacific and
Maritime Continent are essential to cause a significant precipitation deficit
in the western Canadian Prairies. Warm SST in the central Pacific causes an
eastward expansion of Pacific warm pool that favours enhanced MJO activity in
the western-central Pacific (Hendon et al., 1999; Marshall et al., 2016). As
shown by the ray-tracing result, the NINO4 also affects the wavenumber of the
quasi-stationary Rossby waves over the source region in the western Pacific.
Under warm NINO4, the wavenumbers tend to be smaller due to stronger westerly
winds
in the source region and these waves can propagate northeastward into western
Canada. Conversely, from May to August under cold NINO4, the westerly
flow is weaker, and the
meridional vorticity gradient is stronger in the subtropics near the source
region. These mean flow conditions correspond to waves with lager wavenumbers
that cannot propagate across the dateline.</p>
      <p id="d1e1370">In the year 2015, the SST anomaly in the Pacific (e.g., ENSO, NPM) coincided
with the anomalous ridge on the west coast of Canada. This positive GPH
anomaly was associated with the strong negative MJO4 indices, it then caused
a blocking pattern, and suppressed precipitation in the Canadian Prairies in
the early summer through the mechanism discussed above. Although the El Niño
continued to strengthen in July and August 2015, the active convection
associated with MJO in the western Pacific propagated eastward into the
central Pacific. As the convection in the<?pagebreak page5065?> western Pacific/Maritime Continent
waned, the precipitation in the Canadian Prairies returned to slightly above
normal in July.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusions</title>
      <p id="d1e1380">The cause of the 2015 summer precipitation deficit in the western Canadian
Prairies is investigated in relation to atmospheric circulation anomalies,
SST, and the intraseasonal tropical convection oscillation, MJO. The drought in
western Canada is immediately related to an anomalous upper-level ridge that
persisted over the west coast of Canada and Alaska since fall 2014. This
ridge was likely associated with a developing El Niño that was enhanced by
the MJO.</p>
      <p id="d1e1383">In general, MJO-4 indices demonstrated significant correlation with the
meteorological drought over the Canadian Prairies from May to August when the
SST in the central Pacific is warm (NINO4 &gt; 0), which also
corresponds to a stronger MJO amplitude in boreal summer. Our study
discovered that MJO phase/strength is connected to the anomalous ridge over
western Canada through the propagation of stationary Rossby waves from the
western Pacific when NINO4 is positive. Though seasonally MJO is weaker in
summer, the spring and early summer MJO amplitudes are larger than normal
when the central Pacific SST is warmer than normal (NINO4 &gt; 0).
The teleconnection between the Canadian Prairies precipitation deficit and
MJO is stronger when NINO4 is positive. The underlying cause of this
significant correlation between MJO-4 indices and the prairie precipitation
in May–August is a stationary Rossby wave train originating from the
Maritime Continent and western Pacific which propagates into Canada. The
ray-tracing experiments show the main difference between a warm phase of
NINO4 and a cold phase is the changes in stationary Rossby wave wavenumber
over the source region. Under NINO4 &gt; 0.5 May–August
conditions, the total wavenumber is about 4 and can propagate into western
Canada if the waves in the experiments are oriented relatively
zonally. Compared to NINO4 &gt; 0.5, NINO4 &lt; <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula>
corresponds to a weaker zonal wind and stronger meridional gradient of
absolute vorticity in the subtropics of the source region
(140–150<inline-formula><mml:math id="M84" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E). Hence, the wavenumbers of stationary Rossby waves
from the source region under NINO4 &lt; <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn></mml:mrow></mml:math></inline-formula> are larger (about 6),
and these waves fail to reach the western hemisphere. The intra-seasonal
predictability of the growing season precipitation in the Canadian Prairies
can be potentially improved by including the MJO amplitude and phase factors
for medium-range and intra-seasonal projection in addition to the ENSO effect especially
when the central-Pacific SST is warm.</p>
</sec>

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

      <p id="d1e1419">All the data used in this study are publicly available. For
the atmospheric circulation field, both the ERA-Interim dataset (ECMWF, 2017)
and the NCEP Reanalysis (NOAA NCEP, 2017) are publicly available through
their corresponding institutions. The SST dataset ERSST v4 (NOAA, 2017a) and
the SST related NINO4 index (NOAA, 2017b) are publicly available through the
NOAA website. The precipitation dataset CMAP (NOAA CPC, 2017a) can be
accessed publicly through the NOAA website. The MJO index from the NOAA CPC
of the USA (NOAA CPC, 2017b) is available through the NOAA CPC's MJO website.
The MJO index (Bureau of Meteorology of Australia, 2017) and archives on MJO
are hosted by the Bureau of Meteorology of Australia. MEI (NOAA, 2017c) is
publicly available online through the NOAA website. The Interpolated Outgoing
Longwave Radiation (OLR) dataset (NOAA, 2017d) is also available online.</p>
  </notes><notes notes-type="authorcontribution">

      <p id="d1e1425">ZL and YL conceived of the presented idea. ZL developed the theory and performed the computations and analyses.
BB and AM verified the analytical methods. YL supervised the findings of this
work. LS improved the texts and figures. All the authors discussed the results
and contributed to the final manuscript.</p>
  </notes><notes notes-type="competinginterests">

      <p id="d1e1431">The authors declare that they have no conflict of
interest.</p>
  </notes><notes notes-type="sistatement">

      <p id="d1e1437">This article is part of the special issue “Understanding and
predicting Earth system and hydrological change in cold regions”. It is not
associated with a conference.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e1443">We gratefully acknowledge the Natural Sciences and Engineering Research
Council of Canada (NSERC) for funding the Changing Cold Regions Network
(CCRN) through their Climate Change and Atmospheric Research (CCAR)
initiative. Zhenhua Li is supported by the Probing the Atmosphere of the High
Arctic project sponsored by the NSERC. Yanping Li gratefully acknowledges the
support from the Global Institute of Water Security at the University of
Saskatchewan. This research is also supported by Environment and Climate
Change Canada (ECCC). We gratefully acknowledge the support from the Changing
Cold Region Network (CCRN), Global Water Future (GWF) and Global Institute of
Water Security (GIWS) at the University of Saskatchewan.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?> Edited by: John Hanesiak<?xmltex \hack{\newline}?> Reviewed by: two
anonymous referees</p></ack><ref-list>
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    <!--<article-title-html>Combined impacts of ENSO and MJO on the 2015 growing season drought on the Canadian Prairies</article-title-html>
<abstract-html><p>Warm-season precipitation on the Canadian Prairies plays a crucial role in
agricultural production. This research investigates how the early summer 2015
drought across the Canadian Prairies is related to the tropical Pacific
forcing. The significant deficit of precipitation in May and June 2015
coincided with a warm phase of the El Niño–Southern Oscillation (ENSO) and a
negative phase of Madden–Julian Oscillation (MJO)-4 index, which favour a
positive geopotential height (GPH) anomaly in western Canada. Our further
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atmospheric circulation anomalies over western Canada teleconnected with the
lower boundary conditions in the tropical western Pacific. Our results
indicate that MJO can play a crucial role in determining the summer
precipitation anomaly in the western Canadian Prairies when the equatorial
central Pacific is warmer than normal (NINO4&thinsp;&gt;&thinsp;0) and MJO is more
active. This teleconnection is due to the propagation of a stationary Rossby
wave that is generated in the MJO-4 index region. When the tropical
convection around MJO-4 index region (western tropical Pacific, centred over
140°&thinsp;E) is more active than normal (NINO4&thinsp;&gt;&thinsp;0), Rossby
wave trains originate from the western Pacific with wavenumbers determined by
the background mean wind and meridional absolute vorticity gradient. Under
warm NINO4 conditions waves are generated with smaller wavenumbers compared
to cold NINO4 conditions. These waves under warm NINO4 can propagate into the
mid-latitudes over North America, causing a persistent anomalous ridge in the
upper level over western Canada, which favours dry conditions over the
region.</p></abstract-html>
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