Characteristics and evolution of atmospheric circulation patterns during Meiyu over the Jianghuai...
Transcript of Characteristics and evolution of atmospheric circulation patterns during Meiyu over the Jianghuai...
Asia-Pacific J. Atmos. Sci., 48(2), 145-152, 2012
DOI:10.1007/s13143-012-0014-6
Characteristics and Evolution of Atmospheric Circulation Patterns during Meiyu
over the Jianghuai Valley
Danni Liu1, Jinhai He
1, Yonghong Yao
2, and Li Qi
1
1Jiangsu Key Laboratory of Meteorological Disaster of Ministry of Education, Nanjing University of Information Science and Technology, Nanjing, China2School of the Atmospheric Science of Nanjing University, Nanjing, China
(Manuscript received 19 April 2011; revised 25 November 2011; accepted 18 December 2011)© The Korean Meteorological Society and Springer 2012
Abstract: This study focuses on the evolution of large-scale
circulations before and after the beginning of the Meiyu and analyzes
the formations of the typical vertical circulation pattern associated
with Meiyu and its relationship with the Meiyu rainband. Results
show that the typical vertical circulation pattern during the Meiyu
season is characterized by the "two-leg"-type pattern in the vorticity
field, a typhoon eye-like structure of the equivalent potential tempera-
ture field, as well as the sharp gradient of the equivalent potential
temperature zone, i.e., the Meiyu front are typically presented in the
Meiyu season. Tracking its evolution process, we find that the typical
vertical circulation pattern is built at late March and early April
along with the rainband locating at the area south to the Yangtze
River. This typical pattern and the rainband both advance northward
affecting Jianghuai valley since the beginning of Meiyu. Moreover,
the typical vertical circulation pattern derived from Meiyu season has
been formed in April and corresponds to the reverse of the land-sea
thermal contrast between the Eastern Asia and western Pacific Ocean,
demonstrating the close relationship of the movement between the
rainband and the march of the East Asian subtropical summer
monsoon.
Key words: Meiyu, circulation pattern, East Asian subtropical summer
monsoon
1. Introduction
Meiyu is a long-lasting rainy season characterized by a quasi
stationary rainband over the middle and lower reach of the
Yangtze River from mid-June to early or mid-July in eastern
China (Zhu et al., 2000). The rainy season, Meiyu, named as
Changma in Korea and Baiu in Japan, is one of the most prom-
inent seasonal climatological phenomena. Approximately, the
Meiyu season starts on the 17th of June and ends on the 8th of
July, lasting about 22 days. As a major rainfall season in east
China, Meiyu is on the spotlight because of its relationship
with East Asia monsoon (Tao et al., 1987; Matsumoto, 1988,
1992; Lee et al., 1992; Kang et al., 1999; Zhao et al., 2007).
The breakup of the Meiyu season is closely related to the
periodical northward migration of East Asia summer monsoon.
The East Asia subtropical summer monsoon and the South
China Sea (SCS) summer monsoon are two branches of the East
Asia summer monsoon. The East Asian subtropical summer
monsoon and its associated rainband were built at the end of
March and the beginning of April. The onset of the subtropical
summer monsoon is characterized by the reverse of the me-
ridional wind, whereas the onset of the SCS is representative of
the reverse of the zonal wind. Controversy exists on whether
the shift of the Meiyu rainband is related to the East Asian
subtropical monsoon or SCS summer monsoon. Chen et al.
(2004) indicated that the subtropical rain season, Meiyu, is
different from the tropical rain season but they occur in
sequence from spring to summer. The rainband associated with
the subtropical summer monsoon develops in early April to the
south of Yangtze River, and it shifts northward with the
migration of the subtropical High after the onset of the SCS
summer monsoon. Chen et al. (2008) and Zhao et al. (2008)
and He et al. (2008) found similar conclusions and showed
that the shift of the rainband is associated with the seasonal
northward march of the East Asian subtropical monsoon. On
the other hand, some studies have shown that the large-scale
rainband affecting the eastern China is formed after the onset
of the SCS summer monsoon, and the rainband advanced
northward in sequence of time (e.g., Liu et al., 1997; Lian et
al., 2007) as a result of the seasonal migration of East Asia
summer monsoon. The main purpose of this study is to further
investigate whether the advance of the subtropical summer
monsoon or the march of the tropic summer monsoon leads to
the onset of Meiyu season.
Ding et al. (2007) showed that the wind fields at both 850
and 200 hPa displayed the similar seasonal process with that of
Meiyu rainband. It will be helpful by analyzing the formation
processes of both the rainband and the typical circulation pat-
tern around the Meiyu season to examine the relationship bet-
ween the Meiyu rainband and the East Asia summer monsoon.
Features of atmospheric circulations in the midst of the Meiyu
season have been extensively investigated in the past (e.g.,
Chang et al., 1998; Ding et al., 2007; Yang et al., 2010). Few
studies have investigated atmospheric circulations associated
with the rainband before the onset of Meiyu, specially, on the
difference between the vertical distribution of the vorticity
field. We will compare the seasonal variations of the circulation
Corresponding Author: Jinhai He, Jiangsu Key Laboratory of Me-teorological Disaster of Ministry of Education, Nanjing Universityof Information Science and Technology, 219 NinLiu Road,Nanjing 210044, China.E-mail: [email protected]
146 ASIA-PACIFIC JOURNAL OF ATMOSPHERIC SCIENCES
before and after the onset of the Meiyu, and detect the typical
circulation pattern of Meiyu qualitatively. To explore the rela-
tionship between the East Asia summer monsoon and the
seasonal advancement of the rainband in the east of China, vari-
ations of the large scale fields such as the vortex field and
vorticity field as well as temperature and humidity fields before
and after the beginning of Meiyu will be examined in details.
Both typical pattern in atmospheric circulations during the
Meiyu season and the formation date of the typical circulation
pattern will be presented in the study as well. Eventually the
relationship between the onset of the East Asia monsoon and the
seasonal process of the rainband will be discussed in this paper.
2. Data and methodology
The datasets used in this study include daily atmospheric
fields in the NCEP/NCAR reanalysis, and daily precipitation
data at 753 stations in China and Meiyu parameters in the
middle-lower reach of the Yangtze River determined from the
National Meteorological Information Center of China from 1954
to 2001. According to Meiyu parameters, the Meiyu season
starts on 18th, June.
The five provinces, Zhejiang, Hubei, Anhui, Jiangsu and
Shanghai, are selected to represent the region of the middle-
lower reach of Yangtze River from 28oN to 35oN, and 110oE to
122oE, i.e., Jianghuai valley. According to dates of Meiyu
onset provided by these provinces, the mean onset date of
Meiyu has been estimated. Due to diversity in the definition of
Meiyu onset among the provinces, the Meiyu onset dates could
be remarkably different. For example, the onset date of Meiyu
in 1987 provided by two neighboring Jiangsus and Anhui
provinces is on the17th of June and on the 30th of June respect-
ively. If the differences of the Meiyu onset date between five
provinces are smaller than 5 days for a certain year, this year
will be selected as a candidate for use. Otherwise, the mean
Meiyu onset date over will be unreliable and this year is not
selected for use. For example, the year of 1987 is not qualified
for use. Furthermore, the mean Meiyu onset dates of the above
selected years are compared with that from the National Mete-
orological Information Center of China. A year with the differ-
ence between the two onset dates of Meiyu smaller (larger)
than 5 days is considered as a consistent (inconsistent) year.
Table 1 lists all consistent and inconsistent years. For these
consistent years, the mean atmospheric circulation is obtained
by averaging circulations in the 10 days after the onset of
Meiyu. It is found that the mean atmospheric circulation within
10 days after the onset of Meiyu is similar to that during the
entire Meiyu season. Therefore, the mean Meiyu onset date can
be considered as a base point for detecting the evolution of large
scale Meiyu circulation. The formation of typical circulation
patterns during the Meiyu season and their evolution processes
will be investigated based on pentad mean data.
3. Characteristics of precipitation, vorticity and diver-gence before and after the onset of Meiyu
The formation of the large-scale rainband in Jianghuai valley
is considered as the beginning of the Meiyu season. Figure 1
shows that the maximum precipitation region, i.e., the main
rainband, is located at 21oN before the onset of Meiyu. The
main rainband moves northward to the Jianghuai basin after
Meiyu, about at 30oN with the secondary maximum precipi-
tation center at HuaNan in China.
The large-scale vertical motion can be forced by the conver-
gence, which transports the moisture to the precipitation area.
Figures 2a-b show that, the strong convergent area is exactly
consistent with the maximum precipitation area. Both the maxi-
mum precipitation and the strong convergent area are located to
south of the Yangtze River before the Meiyu, and then march
simultaneously over the middle-lower reach of the Yangtze
River valley after Meiyu. To the east of 115oE, the heavy
rainfall region matches the strong convergent region well. To
the west of 115oE, there is no strong convergent area corres-
ponding to the heavy rainfall area occurring there. However,
the divergence of the meridional wind component, with the
magnitude of −4 × 10−6, is consistent with this patch of heavy
rainfall area (Fig. 2d). This might suggest that the evolution of
the main rainband depends on the divergence of the meridional
wind component.
The evolutions of the divergence field of the zonal and
meridional components of winds before and after the onset of
Meiyu (10 days before and 10 days after) are shown in Figs.
3a-b. It is found that the divergence of the zonal wind and the
convergence of the meridional wind occur at the low level at
the same time. Both the intensity of the convergence and the
divergence start to increase 5 days before the onset of Meiyu
and reach their maximum value 1 day after the onset of Meiyu.
Table 1. Consistent and inconsistent years.
31 consistent years 17 inconsistent years
1955, 1956, 1957, 1959, 1960, 1961, 1962, 1963, 1964, 1967, 1968, 1969, 1970, 1972, 1973, 1974, 1975, 1976, 1977, 1979, 1980, 1981, 1983, 1984, 1986, 1988, 1990, 1995, 1997, 2001
1954, 1958, 1965, 1966, 1971, 1978, 1982, 1987, 1989, 1991, 1992, 1993, 1994, 1996, 1998, 1999, 2000 Fig. 1. Meridional variations of 10 day mean diurnal precipitation
(mm d−1) before Meiyu (−10d) and after Meiyu (10d) from 110oE to120o
E.
31 May 2012 Danni Liu et al. 147
The magnitude of convergence of the meridional wind is larger
than that of divergence of the zonal wind, resulting in the occur-
rence of the convergence at the low level. The variations of the
divergence are comparatively complex at the high level. The
intensities of divergence and convergence start to decrease 4
days before the onset of Meiyu. The convergence of the merid-
ional wind reduces sharply 2 days before Meiyu onset, or even
turns to the divergence with its intensity larger than that of the
zonal wind. After Meiyu onset, the divergence of the meridional
wind changes from positive values to negative values process-
ively, but its divergent intensity is smaller than that of the zonal
wind. Therefore, the net divergent intensity is presented as
positive values at the high level. It is the enhancement of the
convergence of the meridional wind that leads to the net
convergent intensity at the low level. Meanwhile, the remark-
able reduction in the convergent intensity of the meridional
Fig. 2. Divergence (Solid line, unit is 10−6 s−1) at 850 hPa, precipitation (shaded area, unit is mm d−1), and wind vector (arrow) at 850 hPa before (a),and after (b) Meiyu ; divergence of the meridional wind component (solid line, unit is 10−6
s−1
) at 850 hPa, precipitation (Shaded area, unit is mm d−1
),and wind vector (arrow) at 850 hPa before (c) and after (d) Meiyu.
Fig. 3. (a) Daily variations of the 850 hPa divergence (× 10−6
s−1
) averaged over the region of 28oN to 32
oN, and 110
oE to 120
oE. D1 represents the
divergence of the zonal wind component, D2 represents the divergence of the meridional wind component, and D1 + D2 represent the totaldivergence. (b) is same as (a) except for 200 hPa.
148 ASIA-PACIFIC JOURNAL OF ATMOSPHERIC SCIENCES
wind and the persistent divergence of the zonal wind produce
the intensified divergence at the high level. The changes of the
meridional wind before and after the onset of Meiyu play a
leading role in the variation of the divergent field and con-
tribute significantly to the precipitation. Two separated positive
vorticity zones are always found at the low level vorticity field
before and after the onset of Meiyu. The northeastern zone is
located over the Inner Mongolia Plateau without the apparent
changes, whereas the southern zone of the positive vorticity
remains to the south of the Yangtze River and advances north-
ward to the Jianghuai Valley, which coincides with the shift of
the maximum precipitation zone (Figure not shown).
4. Vertical structures and evolution of circulation, mois-ture and temperature during the Meiyu
The characteristics and evolution of vertical circulation in
the Meiyu season are revealed by the cross section analysis
averaged from 110ºE to 120ºE during the Meiyu season (Fig.
4f), three major positive vorticity zones are located at the low-
middle level of the troposphere, centered at the South China
Sea (SCS, 10ºN to 20ºN), the Jianghuai valley (25ºN to 35ºN)
and the Inner Mongolia Plateau (north to 42ºN), respectively.
The positive vorticity zone at the SCS represents the activity of
the SCS monsoon and the height of its core (> 3 × 10−6 s−1)
Fig. 4. Meridional cross section of 5 day mean temperature in oC (dash line), specific humidity in g kg−1 (solid line) and vorticity in10−6 s−1 (shaded)averaged between 110
oE and 120
oE for the period of (a) from 11
th to 12
th pentad, (b) from 22
nd to 23
rd pentad, (c) from 26
th to 27
th pentad, (d) from
28th to 29th pentad, (e) before Meiyu, and (f) after Meiyu.
31 May 2012 Danni Liu et al. 149
hardly reaches the middle level of the troposphere. The positive
vorticity zones at the Jianghuai valley and Inner Mongolia
Plateau penetrate the entire troposphere. These two zones are
separated by a negative vorticity zone at the low level but
merge at the high level to form an integrated part. This pattern
of the vorticity field is nicknamed as “two leg pattern”. One of
the two legs refers to the positive vorticity zone at the Jianghuai
valley, and the other at the Inner Mongolia Plateau, termed as
the south leg and the north leg respectively. The south leg
corresponds to the interface of the Meiyu front between the
upward warm air mass and the downward cold air mass. The
south leg of the positive vorticity tilts northward with height,
indicative of a baroclinic structure with the positive vorticity at
the low level and the negative vorticity at the middle and high
level of the troposphere. The baroclinic structure implies the
juxtaposition of the Meiyu front at the low level with the sub-
tropical high at the middle level, and the south Asia subtropical
high at the high level of troposphere (Zhu et al., 2000). The
north leg of the two leg pattern manifests itself as a less
baroclinic structure.
Our results in Fig. 5 are broadly consistent with features of
temperature field and moisture field in the meiyu season sum-
marized in Ding et al. (2007). Figure 5 shows that a high
specific humidity zone lays inside the Meiyu region at the low
level of the troposphere. From the meridianal cross section, the
southern leg of the “two leg pattern” is accompanied by both
temperature ridge and humidity ridge through the entire tropo-
sphere. The northern leg of the “two leg pattern” is also
Fig. 5. Meridional cross section of 5-day mean θse (dash line, unit is K) transected between 110
oE and 120
oE for the period of (a) from 11
th to 12
th
pentad; (b) from 22nd to 23rd pentad; (c) from 26th to 27th pentad; (d) from 28th to 29th; (e) before Meiyu; (f) after Meiyu .The solid line represents θse
equal to 328K. The dense θse zone with its value smaller than 12K is shaded.
150 ASIA-PACIFIC JOURNAL OF ATMOSPHERIC SCIENCES
collocated with a weak temperature ridge at lower troposphere.
This distribution of temperature makes the Meiyu region sitting
in a cold temperature trough at the low level. The occurrence of
the weak temperature ridge implies a warm and moist air mass
located to south of the “south leg” positive vorticity zone. This
feature can be found easily from the field of equivalent poten-
tial temperature (Fig. 5f). The sharply changing zone of θse
(shaded), represents the Meiyu frontal zone. In the Meiyu
season, a low θse zone, located to north of the Meiyu frontal
zone, indicates the existence of a dry and cold air mass. In the
meantime, a high θse zone lies to the south of the Meiyu frontal
zone, acting as a warm and moist air mass. At the flank of the
warm air mass, θse decreases with height at the low level,
indicating that the air there is moist unstable. At the middle
level, θse is homogeneous and reaches a minimum. Then θ
se
increases with height at the upper troposphere. This vertical
structure of equivalent potential temperature resembles the
structure of a typhoon eye (Ding et al., 2007), characterized by
the ridge of the temperature and the ridge of humidity through
the entire troposphere, and the high value of θse
locating to the
south of the Meiyu front. In contrast to the vertical structure of
vorticity, temperature as well as humidity after the onset of
Meiyu, the feature of a “two-leg” pattern in the vorticity field,
a typhoon-eye-like vertical structure at the side of warm and
moist air and a sharp gradient zone in the equivalent potential
temperature field also appear before the onset of Meiyu, but
with their locations situated more south at the low level of the
troposphere (Fig. 5a). And the southern leg in the two-leg
pattern, around 27oN, is quite weak in terms of positive vor-
ticity before the onset of Meiyu, accompanied by a tempera-
ture ridge and a humidity tongue. With the onset of the Meiyu,
the southern leg of the two-leg pattern is enhanced in term of
increased positive vorticity and shifts toward 30oN, with the
consistent progress of both the temperature ridge and the
humidity tongue. The characteristic contour line of θse with the
value of 328 k withdraws to the north, while the sharp gradient
zone of θse shifts from 30oN to 33oN.
Based on the above analysis, the typical circulation pattern
during the Meiyu season is summarized as follows (1) a “two-
leg” pattern in the vorticity field, (2) a typhoon eye-like struc-
ture in the equivalent potential temperature field, and (3) a
sharp gradient zone of θse i.e., the Meiyu front. These promin-
ent features occur around the onset of the Meiyu. How do they
evolve before and after the onset of the Meiyu? The vertical
structure of pentadly mean vorticity, equivalent potential tem-
perature, and their relationships to the Meiyu rainband is
further examined next.
At the end of February (Fig. 4a), the positive vorticity zones
associated with the “two-leg” pattern hang above 850 hPa.
Negative vorticity dominates at the low level in east China,
caused by the stagnant continental high pressure system at the
low level in this region during the winter. A cold and dry air
mass is reflected in the fields of temperature and humidity in
this region, indicating the dominance of a typical winter pattern.
Meanwhile, a warmer and moist air still stays in the tropics.
Starting at the end of March, the southern leg and the northern
leg of the positive vorticity zone (i.e., “two-leg” pattern) extend
downward to the low level, with the eastward migration of the
continental cold high pressure system (Fig. 6a). The “two-leg”
pattern starts to take shape. The southern leg of the positive
vorticity zone hits the ground and moves to the Jianghuai
valley since the middle of April (Fig. 4b). The northern leg of
the positive vorticity zone also hits the ground but still stays to
the north of 42oN. This transition in the positive vorticity zone
indicates the retreat, i.e., the northward migration, of the
continental cold high pressure system in the eastern China and
the reversal of the ocean-land surface pressure contrast between
the eastern Asia and western pacific (Guo, 1983). In the
middle of May, the northward migration of the South Asian
High at the upper level leads to the poleward tilting of the
Fig. 6. (a) The migration of the continental cold high pressure systemat 925 hPa from 8
th pentad to 19
th pentad. The solid circle represents
the center of the continental cold high pressure system, and thenumber with the solid circle represents the time of the pentad, (b)Meridional variations of the mean wind field (stream line), divergence(Solid line, unit is 10−6 s−1), the ridge of the Weastern North PacificHigh (long dashed line) and the negative vorticity (shaded area) at 500hPa from 110o
E to 120oE.
31 May 2012 Danni Liu et al. 151
south leg of the positive vorticity zone with height (Fig. 4c).
With the progression of the Subtropical High (Fig. 6b), the
southern leg of the “two-leg” positive vorticity zone starts
moving northward at the middle level. Meantime, the “two-leg”
positive vorticity zone is stagnant to the south of the Yangtze
River at the low level, resulting in the poleward tilt of the south
leg of the “two-leg” positive vorticity zone. Thus, a strong
baroclinic zone starts to take shape over the Yangtze River,
with the vertical structure of the positive vorticity zone at the
low level and the negative vorticity at the high level (Fig. 4d).
At the same time, another positive vorticity zone forms over
the SCS (South China Sea) and stretches up to the middle level
after the onset of SCS monsoon (Fig. 4d).
Also demonstrated are the temporal variations of equivalent
potential temperature field. In the end of February (Fig. 5a), the
characteristic θse contour line of 328 K, representative of warm,
moist unstable air mass, is located to the south of the Tropic of
Cancer. And a dry and cold air mass, represented by low θse,
dominates the continental area in East China. Meanwhile, a
broad and sharp horizontal θse gradient zone lies to the north of
the characteristic θse line, suggestive of a strong cold air and
thus a winter circulation pattern. At the end of April (Fig. 5b),
the characteristic θse line of 328 K moves northward to the
south of the Yangtze River, a subtropical area. The sharp gra-
dient zone of θse turns narrower and a front or frontal zone
becomes clearer. In the meantime, with the increasing of θse at
the low level, the instability layer extends to 850 hPa. The
smaller value of the equivalent potential temperature locates
around the south and north area of the dense gradient zone of
θse (shaded area in the plot) respectively, with one of the
smallest center over the SCS at the middle level. The larger
value of the equivalent potential temperature locates at the low
level and the high level to the south of the dense gradient zone.
The “saddle” shaped typical structure of equivalent potential
temperature has been formed (Fig. 5c). After the onset of the
SCS monsoon (Fig. 5d), the warm and moist air mass
advances northward, corresponding to the same movement of
the dense gradient zone of θse, affecting the region south to the
Yangtze River and the Jianghuai valley.
Therefore, the winter patterns in the fields of the vorticity,
temperature and humidity start to change in the end of March.
The positive vorticity zone stretches downward to the low level.
The “saddle” shaped equivalent potential temperature is pro-
duced progressively. Corresponding to the eastward shifting of
the weakening continental High (Fig. 6a), the warm air invades
toward the continent in Eastern China (Fig. 5b-f). The circula-
tion pattern of the “two-leg-shape” vorticity structure and the
“saddle” shaped equivalent potential temperature field have
been set up in late April, and the features of the circulation
pattern is consistent with that of the typical pattern during the
Meiyu season. Accordingly, the typical pattern representative
of the onset of the Meiyu has been built since April, and the
typical circulation pattern advances northward with the warm
and moist air mass to affect the region of southern China and
the Jianghuai valley. The circulation patterns presented in the
fields of the vorticity, temperature, and the humidity after the
onset of Meiyu are very similar to their corresponding typical
patterns before the onset of the Meiyu, which has been set up
since April before the onset of Meiyu. This typical pattern
shifts northward right after the onset of the SCS monsoon.
There have been a number of published studies showing that
the set up of the East Asia Summer Monsoon is closely related
to the seasonal reverse of the land-sea thermal contrast between
Eastern Asia and northwestern Pacific (Guo, 1983; Qi et al.,
2007). The vertical distribution of the circulation structure
suggests that, the typical pattern of Meiyu is formed progres-
sively during the rainy season in Southern China and its
formation coincides with the time of the reverse change of the
pressure difference from the positive value to the negative one
between Eastern Asia continent and the northwestern Pacific.
After the onset of the SCS monsoon, the typical pattern ad-
vances northward with the summer monsoon and affects the
south region to the Yangtze River and Jianghuai valley,
accompanied by the northward shift of the rainfall band in
eastern China. Therefore, the typical pattern of the “two-leg”
vorticity, the equivalent potential temperature whose vertical
structure is quite similar to that in a typhoon eye presented after
the Meiyu has been detected since the late March and the early
April. The typical pattern presented during the Meiyu season is
considered as the result of the northward shift of the circu-
lation set up to south of Jianghuai Valley before the onset of
Meiyu. The existence of the typical pattern relating to the
building of the east subtropical summer monsoon is a signal of
the seasonal transition in Eastern China.
5. Summary
In this study, variations of the large scale circulation and the
typical circulation pattern as well as its evolution before and
after the onset of Meiyu have been examined with the analysis
of the cross sections passing through the eastern China. The
typical circulation structure during the Meiyu season is charac-
terized by the “two-leg” vorticity field, and the equivalent po-
tential temperature field whose vertical structure is quite similar
to that in a typhoon eye as well as the sharp gradient zone of
θse (frontal interface or frontal zone). The vertical circulation
structure moves from south before Meiyu to north after the
onset of Meiyu without change. Tracing the formation and the
evolution of pentad mean of the circulation, the result shows
that the transition of the circulation pattern at the end of March
and the early April corresponds to the beginning of the rainy
season in south China. The circulation pattern of “two-leg”
shaped vorticity field, and a typhoon eye-like structure of the
equivalent potential temperature field as well as the sharp gra-
dient zone of θse has been formed on April. The reverse change
of the pressure difference between the East Asia continent and
the northwest Pacific occurs simultaneously. Both the typical
circulation structure and the rainfall band shift northward after
the onset of Meiyu. The spring season is the first stage of the
rainfall season associated with the subtropical monsoon. So we
152 ASIA-PACIFIC JOURNAL OF ATMOSPHERIC SCIENCES
conclude that the seasonal transition of the subtropical monsoon
leads to the onset of Meiyu. The appearance of the typical
circulation pattern with the rainfall band is representative of
the onset of the East Asia subtropical summer monsoon. Both
the precipitation and the circulation pattern move simultan-
eously with the seasonal process of East Asia subtropical
summer monsoon.
Acknowledgements. This study is jointly supported by National
Natural Science Foundation of China (Grant No. 41075068 and
40875044) and National Public Benefit Research Foundation of
China (GYHY200706005).
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