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1.
南海夏季海流的数值模拟 总被引：3，自引：0，他引：3
用一个水平分辨率较高的区域海洋模式计算了中国海的海流。本文给出了南海７月份的上层环流的数值模拟结果。结果表明:在南海北部的陆架区，一支较强的东北向海流穿过台湾海峡流入东海；在海南岛东南和越南沿岸以东海域有一个气旋式的涡旋；南海南部被一个反气旋式的大涡旋所占据。计算得到的这些环流特征与观测结果十分一致。另外，数值模拟结果还显示出，黑潮的一个分支通过巴士海峡的南部进入南海，虽然一部分海水不断被陆架诱导流向东北，但是仍有一部分海水可以一直向西流到海南岛以东海域。 相似文献
2.
The upper layer, wind-driven circulation of the South China Sea (SCS), its through-flow (SCSTF) and the Indonesian through flow (ITF) are simulated using a high resolution model, FVCOM (finite volume coastal ocean model) in a regional domain comprising the Maritime Continent. The regional model is embedded in the MIT global ocean general circulation model (ogcm) which provides surface forcing and boundary conditions of all the oceanographic variables at the lateral open boundaries in the Pacific and Indian oceans. A five decade long simulation is available from the MITgcm and we choose to investigate and compare the climatologies of two decades, 1960–1969 and 1990–1999.The seasonal variability of the wind-driven circulation produced by the monsoon system is realistically simulated. In the SCS the dominant driving force is the monsoon wind and the surface circulation reverses accordingly, with a net cyclonic tendency in winter and anticyclonic in summer. The SCS circulation in the 90s is weaker than in the 60s because of the weaker monsoon system in the 90s. In the upper 50 m the interaction between the SCSTF and ITF is very important. The southward ITF can be blocked by the SCSTF at the Makassar Strait during winter. In summer, part of the ITF feeds the SCSTF flowing into the SCS through the Karimata Strait. Differently from the SCS, the ITF is primarily controlled by the sea level difference between the western Pacific and eastern Indian Ocean. The ITF flow, consistently southwestward below the surface layer, is stronger in the 90s.The volume transports for winter, summer and yearly are estimated from the simulation through all the interocean straits. On the annual average, there is a ∼5.6 Sv of western Pacific water entering the SCS through the Luzon Strait and ∼1.4 Sv exiting through the Karimata Strait into the Java Sea. Also, ∼2 Sv of SCS water enters the Sulu Sea through the Mindoro Strait, while ∼2.9 Sv flow southwards through the Sibutu Strait merging into the ITF. The ITF inflow occurs through the Makassar Strait (up to ∼62%) and the Lifamatola Strait (∼38%). The annual average volume transport of the ITF inflow from the simulation is ∼15 Sv in the 60s and ∼16.6 Sv in the 90s, very close to the long term observations. The ITF outflow through the Lombok, Ombai and Timor straits is ∼16.8 Sv in the 60s and 18.9 Sv in the 90s, with the outflow greater by 1.7 Sv and 2.3 Sv respectively. The transport estimates of the simulation at all the straits are in rather good agreement with the observational estimates.We analyze the thermal structure of the domain in the 60s and 90s and assess the simulated temperature patterns against the SODA reanalysis product, with special focus on the shallow region of the SCS. The SODA dataset clearly shows that the yearly averaged temperatures of the 90s are overall warmer than those of the 60s in the surface, intermediate and some of the deep layers and the decadal differences (90s − 60s) indicate that the overall warming of the SCS interior is a local effect. In the simulation the warm trend from the 60s to the 90s in well reproduced in the surface layer. In particular, the simulated temperature profiles at two shallow sites at midway in the SCSTF agree rather well with the SODA profiles. However, the warming trend in the intermediate (deep) layers is not reproduced in the simulation. We find that this deficiency is mostly due to a deficiency in the initial temperature fields provide by the MITgcm. 相似文献
3.
夏季东亚高空急流与太平洋-日本遥相关型的关系 总被引：1，自引：1，他引：1
利用NCEP/NCAR和NOAA月平均资料,采用奇异值分解方法分析了夏季东亚高空纬向风场和西北太平洋海表温度(SST)的耦合关系,并据此研究了东亚副热带高空急流和太平洋-日本(Pacific-Japan,PJ)遥相关型的可能联系。合成分析结果表明,东亚副热带高空急流正模态年,急流偏南偏强,对流层上层南亚高压增强东进,中层西太平洋副热带高压加强西伸,菲律宾周边海域SST升高,中纬度黑潮延伸体区SST降低,菲律宾海和热带西太平洋地区对流活动偏弱,日本海和黑潮延伸体海区对流活动增强,对应PJ遥相关型的负位相;而东亚副热带高空急流负模态年,急流偏北偏弱,对流层上层南亚高压减弱西退,中层西太平洋副热带高压减弱东撤,菲律宾周边SST降低,中纬度黑潮延伸体区SST升高,菲律宾海和热带西太平洋地区对流活动强盛,日本海和黑潮延伸体海区对流活动减弱,对应PJ遥相关型的正位相。由于夏季东亚副热带高空急流活动与PJ遥相关型存在关联,PJ遥相关型可能是东亚副热带高空急流响应太平洋海温异常的纽带。 相似文献
4.
An overview of a new comprehensive observational study of the Loop Current (LC) in the eastern Gulf of Mexico that encompassed full-depth and near-bottom moorings, pressure-equipped inverted echo sounders (PIES) and remote sensing is presented. The study array was designed to encompass the LC from the Campeche Bank to the west Florida escarpment. This overview centers about principal findings as they pertain to mesoscale dynamics. Two companion papers provide in-depth analyses. Three LC anticyclonic eddy separation events were observed with good 3D spatial coverage over the 2½ year extent of the field study; the three separations exhibited similar processes after the LC had extended into the eastern Gulf. Large scale (∼300 km wavelength, 40–60 day periods) southward propagating meanders developed on the eastern side of the LC over deep (∼3000 m) water that were the result of baroclinic instability between the upper layer meandering jet and lower layer cyclones and anticyclones. The lower layer was only highly energetic during relatively short (∼2–3 months) intervals just prior to or during eddy detachments because of baroclinic instability. The steepening of the meanders lead to a pinch-off of LC eddies. The deep lower-layer eddies, constrained by the closed topography of the southeastern Gulf, propagated westward across the detachment zone and appear to assist in achieving separation. Small scale (∼50–100 km, periods ∼10 days) frontal eddies, observed on the western side of the LC along the Campeche Bank slope, decay over the deep water of the northern part of an extended LC, and have little influence on lower layer eddies, the east side meanders and the eddy detachment processes. 相似文献
5.
基于华南地区60个站点的逐日降水资料及NCEP再分析资料,采用拉格朗日后向气流轨迹模式(HYSPLIT_4.9),分析了1960—2012年PDO (Pacific Decadal Oscillation,太平洋年代际振荡)不同相位期间,华南前汛期锋面和季风降水的水汽输送轨迹、主要源地及不同源地水汽的降水贡献率的差异。结果表明:1)锋面降水阶段,在PDO正相位期间,西太平洋-中国南海-孟加拉湾水汽较多;夏季风降水阶段,在PDO正位相期间,北印度洋-孟加拉湾-中国南海的整层水汽含量较多。2)锋面降水阶段,水汽主要来自西北太平洋与中国南海,在PDO正相位期间,副热带高压位置偏北,使得西太平洋水汽输送路径偏北,有更多水汽向华南输送,有利于华南季风降水形成,降水与PDO呈显著的正相关关系。3)季风降水阶段,在PDO正位相期间,尽管北印度洋-孟加拉湾-中国南海的整层水汽含量大,但并未都输送至华南,故形成的有效季风降水偏少,降水与PDO呈显著的负相关关系。 相似文献
6.
The precipitation over eastern China during January–March 2010 exhibited a marked intraseasonal oscillation (ISO) and a dominant period of 10-60 days. There were two active intraseasonal rainfall periods. The physical mechanisms responsible for the onset of the two rainfall events were investigated using ERA-interim data. In the first ISO event, anomalous ascending motion was triggered by vertically integrated (1000–300 hPa) warm temperature advection. In addition to southerly anomalies on the intraseasonal (10–60-day) timescale, synoptic-scale southeasterly winds helped advect warm air from the South China Sea and western Pacific into the rainfall region. In the second ISO event, anomalous convection was triggered by a convectively unstable stratification, which was caused primarily by anomalous moisture advection in the lower troposphere (1000–850 hPa) from the Bay of Bengal and the Indo-China Peninsula. Both the intraseasonal and the synoptic winds contributed to the anomalous moisture advection. Therefore, the winter intraseasonal rainfall events over East Asia in winter could be affected not only by intraseasonal activities but also by higher frequency disturbances. 相似文献
7.
Prior studies have revealed that,as a part of the Pacific tropical gyre,the South China Sea throughflow(SCSTF) is strongly influenced by the Pacific low-latitude western boundary current(LLWBC).In this study,ocean general circulation model(OGCM) experiments with and without connection to the South China Sea(SCS) were performed to investigate the impact of the SCSTF on the Pacific LLWBC.These model experiments show that if the SCS is blocked,seasonal variability of the Kuroshio and Mindanao Current becomes stronger,and the meridional migration of the North Equatorial Current(NEC) bifurcation latitude is enhanced.Both in seasonal and interannual time scales,stronger Luzon Strait transport(LST) induces a stronger Kuroshio transport combined with a southward shift of the NEC bifurcation,which is unfavorable for a further increase of the LST;a weaker LST induces a weaker Kuroshio transport and a northward shifting NEC bifurcation,which is also unfavorable for the continuous decrease of the LST. 相似文献
8.
本文利用2010—2019年滇中石林县的全球再分析资料，通过HYSPLIT模型的后向轨迹对不同季节和不同高度的水汽来源进行追踪和分析。结果表明：石林县四季的水汽源地和水汽运移路径存在差异。春季水汽主要来源于受高空西风影响的欧亚大陆和非洲北部，夏季水汽主要来源于孟加拉湾，南海和西太平洋海域，秋季水汽主要来源于孟加拉湾—南海和西太平洋，冬季主要来源于欧亚大陆和非洲北部的高空西风、孟加拉湾海域。石林县的水汽通道有阿拉伯海和孟加拉湾—南海、西太平洋、欧亚非大陆、局地五条水汽通道，且春夏秋冬四季的不同高度层的水汽输送通道和水汽贡献率存在较大差异。 相似文献
9.
《Dynamics of Atmospheres and Oceans》2009,46(3-4):165-186
Recent observations in the Sea of Japan show evidence of convection to a depth of roughly 1000 m in the winter of 2000, situated along the polar front. Numerical simulations have shown that this deep mixing is associated with both ageostrophic frontal circulations and pre-existing larger-scale downwelling regimes. The downwelling regimes appear to be a result of interactions between frontal meandering and deep circulation in this basin over bottom topography anomalies. The coupling between the frontal dynamics and the deep circulation are explored by analogy to atmospheric frontal circulations through the semigeostrophic Sawyer–Eliassen equation, solved numerically for the case of the Sea of Japan. As in the atmospheric case, a vertical coupling between the upper and lower circulations can produce a localized region of downwelling that can be conducive to deeper mixing than that forced solely from surface fluxes. 相似文献
10.
《Dynamics of Atmospheres and Oceans》1988,12(2):173-189
The Kuroshio Front to the east of Honshu, Japan, commonly has a double structure. The front consists of three main parts: the temperature front at its northern edge, the density front at its southern edge and the inside zone between them. In a previous paper suggested that the structures of the density front in November, 1984, of the inside zone in July, 1983, and of the inside zone in November, 1984, indicate the generation stage, the mature stage, and the decay stage of the double structure of the Kuroshio Front, respectively. Also, it was suggested that there is a mechanism which draws deeper thermocline water beneath the Kuroshio into the surface layer of the frontal zone. By using the same data taken in 1983 and 1984, we have conducted detailed water mass analysis with special reference to the double structure of the Kuroshio Front. The results, presented in this paper, support the arguments presented earlier. 相似文献
11.
Jianhong WANG Meiqi LI X.San LIANG Xing WANG Feng XUE Mo PENG Chunsheng MIAO 《大气科学进展》2018,35(7):826-838
The asymmetrical structure of typhoon-induced ocean eddies(TIOEs) in the East China Sea(including the Yellow Sea)and the accompanying air–sea interaction are studied using reanalysis products. Thirteen TIOEs are analyzed and divided into three groups with the k-prototype method: Group A with typhoons passing through the central Yellow Sea; Group B with typhoons re-entering the sea from the western Yellow Sea after landing on continental China; and Group C with typhoons occurring across the eastern Yellow Sea near to the Korean Peninsula. The study region is divided into three zones(Zones Ⅰ, Ⅱ and Ⅲ) according to water depth and the Kuroshio position. The TIOEs in Group A are the strongest and could reverse part of the Kuroshio stream, while TIOEs in the other two groups are easily deformed by topography. The strong currents of the TIOEs impact on the latent heat flux distribution and upward transport, which facilitates the typhoon development. The strong divergence within the TIOEs favors an upwelling-induced cooling. A typical TIOE analysis shows that the intensity of the upwelling of TIOEs is proportional to the water depth, but its magnitude is weaker than the upwelling induced by the topography. In Zones Ⅰ and Ⅱ, the vertical dimensions of TIOEs and their strong currents are much less than the water depths.In shallow water Zone Ⅲ, a reversed circulation appears in the lower layer. The strong currents can lead to a greater, faster,and deeper energy transfer downwards than at the center of TIOEs. 相似文献
12.
Barrier layer in the South China Sea during summer 2000 总被引：2，自引：0，他引：2
Lili Zeng Yan Du Shang-Ping Xie Dongxiao Wang 《Dynamics of Atmospheres and Oceans》2009,47(1-3):38-54
Using temperature–salinity profiles obtained from a cruise in summer 2000, the structure and formation of the barrier layer (BL) in the South China Sea (SCS) are investigated. Fresh water flux, ocean circulation, and wind stirring are important for BL formation, depending on regions. In the eastern SCS, Philippine mountains induce heavy rainfall, resulting in a fresh water cap at the surface and the formation of a thick wide spread BL. In the northwestern basin on the lee of the Annam Cordillera range, by contrast, a rain shadow reduces fresh water flux, which along with wind-induced upwelling, prevents the BL forming. Southeast of Vietnam, a thick BL forms as the Mekong River plume is advected by the northeastward western boundary current and its offshore extension. In the southeastern basin, the surface water is mixed deeply under the strong southwesterly monsoon, unfavorable for the BL formation despite heavy rainfall. In the Luzon Strait, the east/southeastward surface Ekman drift carries fresh SCS surface water, riding on the intruding Kuroshio meander that carries well-mixed, warm and saline water. The vertical overlapping of these two water masses gives rise to a thick BL. 相似文献
13.
一次冬季江淮气旋逗点云区的雷达回波和气流结构分析 总被引：2，自引：0，他引：2
2016年2月12—13日,受冷空气和江淮气旋暖锋锋生影响,山东出现一次极端暴雨雪天气过程,全省有42个站的降水突破同期历史记录。采用多种观测以及WRF模式模拟的热力学变量,基于拉格朗日方法的气流轨迹模式(HYSPLIT v4.9),分析了气旋逗点云区云系的演变特征、降水不同阶段气旋逗点云区气流结构和轨迹特征。结果表明:(1)江淮气旋逗点云区由4条带状回波合并发展形成,气旋形成后降水回波呈气旋式旋转、拉长,形成多条中尺度强降水带。(2)降雨阶段气旋逗点头从下到上主要由来自东海、黄海、日本海或内陆的边界层气团,来自中国南海和中南半岛的暖湿气团以及来自西亚和东欧的干冷气团组成。气旋逗点头内有3个降水区:北部和南部暖湿气团浅薄、层结稳定,为层状云降水区;中部暖湿气团深厚,中高层有条件性不稳定发展,为深厚的对流云降水区。气旋逗点头中南部的干冷空气来自高层的西亚气团,而剖面北部有来自中层(即青藏高原东部气团)的干冷空气,气团明显变性,对降水贡献大。(3)降雪阶段气旋逗点头从下到上主要由西伯利亚气团、东海气团、南海气团和孟加拉湾气团叠置而成。气旋逗点头西部层状降水区分两部分:北部为降雪区,南部为降雨区。降雪与降雨阶段的明显差别是冷湿的东海气团下面是否有西伯利亚冷气团。降雪区西伯利亚气团上空东海气团深厚,南海气团浅薄;降雨区南海气团深厚,东海气团浅薄。 相似文献
14.
Conventional surface data and quantitative estimations of precipitation are used to document the occurrence and spatial distribution of severe weather phenomena associated with deep moist convection over southeastern South America.Data used in this paper are 24-hour rainfall, maximum hourly gusts and present weather reports from the surface station network for Argentina to the north of 40°S and cover the period 2000–2005. Hourly rainfall estimated with the CMORPH technique (CPC MORPHing technique, R. J. Joyce et al., 2004) is included in the analysis in order to increase the density of the precipitation database from January 2003 to December 2005. Extreme events are detected by means of a 95th-percentile analysis of the 24-hour rainfall and wind; values greater than 30 mm and 25 m s?1 respectively are considered extreme in the study area. These results are related to the presence of deep convection by considering the 235 K and 218 K cloud shield evolution in Geostationary Operational Environmental Satellite-12 Infrared (GOES-IR) imagery evaluated by the Forecasting and Tracking of Cloud Cluster (FORTRACC) technique. Rainfall above 30 mm day?1 and present convection-related weather events tend to occur in the northeast of the country.Finally, an analysis is made of the relationship between severe phenomena and the location and lifecycle of Mesoscale Convective Systems (MCSs) defined by the 218 K or 235 K levels. According to the reports, favorable locations for severe weather concentrate to the northeast of the cloud shield anvil centroid although most of the cases are found in the northwest. This feature can be seen in systems with anvil areas larger than 250,000 km2 in association to the predominant mid-level wind shear direction from the northwest over the area. Moreover, systems with centers located north of 30°S present a more circular shape while those to the south are more elongated with a NW–SE main axis clearly related to the presence and interaction with frontal zones over the area. Most of the events occur previous to the moment when the systems reach their maximum extension, between 2 and 10 h after the initiation of the system depending on the size of the MCSs. 相似文献
15.
A. G. Andreev 《Russian Meteorology and Hydrology》2010,35(9):633-640
The interannual variations of the sea level at the coastal stations of the Sea of Japan and of the water discharge through
the Korea (Tsushima) Strait are studied. It is demonstrated that the interannual variations of the water discharge through
this strait are determined by the water discharge of the Oyashio (in the subarctic Pacific) and the Kuroshio (in the East
China Sea) currents and by the zonal wind stress component over the Sea of Japan in winter period. It is revealed that the
variations in the East China Sea water transport through the Korea (Tsushima) Strait cause the interannual variations of the
dissolved oxygen content in intermediate (500 m) and deep (1000 m and more, σθ = 27.35) waters of the Sea of Japan. 相似文献
16.
Using the regional climate model RegCM4.4.5, coupled with the land model CLM4.5, we investigated the effects of springtime soil moisture in the Indochina Peninsula on summer precipitation over the South China Sea and its surrounding areas in 1999. Results have indicated that there exists positive correlation between soil moisture and summer precipitation over the western Pacific Ocean and negative correlation between soil moisture and summer precipitation over the eastern Indian Ocean. Summer precipitation in the South China Sea and its surrounding areas responds to springtime soil moisture in the Indochina Peninsula (the northwest region is critical) because general atmospheric circulation is sensitive to the near-surface thermodynamic state. Increased (decreased) soil moisture would result in decreased (increased) local surface temperatures. Latitudinal, small-scale land–sea thermal differences would then result in northeasterly wind (southwesterly wind) anomalies in the upper layer and southwesterly wind (northeasterly wind) anomalies in the lower layer, which strengthen (weaken) monsoon development. As a result, precipitation would enter the Western Pacific region earlier (later), and water vapor over the eastern Indian Ocean would enter the South China Sea earlier (later), causing a precipitation reduction (increase) in the eastern Indian Ocean and increase (reduction) in the Western Pacific. 相似文献
17.
In the past three decades, the strongest central Pacific (CP) El Niño event was observed in 2009–2010 by satellites. When intensity of this CP El Niño reached its maximum, large diurnal variations of sea surface temperature (SST) were also observed from tropical atmosphere ocean moorings in the central equatorial Pacific. Solar radiation in the equatorial central Pacific is larger than 140 W/m2, which leads to the amplitude of diurnal cycle of SST primarily determined by large-scale wind patterns. Intraseasonal westerly wind events (WWEs) can lead to an eastward displacement of the warm pool and also can weaken the trade winds in central Pacific. When the occurrence of equatorial WWEs is more than 20 days in a month, monthly mean wind speed in central equatorial Pacific has high possibility of wind speed less than 3 m/s, thus has pronounced diurnal cycle of SST. The diurnal cycle of SST will rectify daily mean SST. Reduced mixing at the base of the mixed layer and suppression of entrainment due to the accumulated effect of diurnal cycle may lead to warmer SST in the following month. This study suggests the occurrence of more diurnal SST events may contribute to the increasing intensity of the CP El Niño events. 相似文献
18.
《Atmospheric Science Letters》2002,3(1):15-24
The development of Tropical Cyclone Diana (1984) is simulated with a mesoscale model using 1.2 km grid spacing over a regional-scale (>1000 km) domain in the first known experiment of this kind. With only a synoptic-scale disturbance in the initial conditions, the model first develops a mesoscale convective system along a remnant frontal zone, which yields a mesoscale vortex. After a period of quiescence, banded convection organizes about the vortex from isolated, grid-resolved cells, with the system becoming warm-core and intensifying into Tropical Storm Diana. 相似文献
19.
Spatial and Temporal Variations of Tropical Cyclones at Different Intensity Scales over the Western North Pacific from 1945 to 2005 
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下载免费PDF全文 The tropical cyclone （TC） track data provided by the Joint Typhoon Warning Center （JTWC） of the U.S. Navy over the western North Pacific （including the South China Sea） from 1945 to 2005 are employed to analyze the temporal and spatial variations of TCs of different intensity scales. Most of the TCs occurred between 15° and 25°N, from the northern part of the South China Sea to the eastern part of the Bashi Channel until near 140°E. Most of the severe and super typhoons occurred over waters from the eastern part of the Bashi Channel to about 140°E. The TCs in a weakening or steady state take up a weak majority in the area west of 123°E and north of 20°N; those in an intensifying or steady state are mostly found in the area east of 123°E and south of 20°N. For severe tropical storms, typhoons, severe typhoons, and super typhoons, their average decaying rates are all greater than the respective average growing rates; for tropical storms, however, the average decaying rate is smaller than the average growing rate. Generally speaking, the stronger the TC, the faster the intensification （weakening） is. The percentage of weak TCs is higher in June to August while that of strong TCs is higher in September to November. There are annual, interannual, and interdecadal variations in the observed number （every 6 h） and frequency of TCs at different intensity scales. As far as the long-term trend is concerned, the frequency and observed number of tropical storms have a significant linear increase, but the averaged intensity and number of TCs of other intensity categories do not exhibit such a significant linear trend. In E1 Nifio years, the number and percentage of super typhoons are significantly higher, while the total number of tropical storms, severe tropical storms, typhoons, and severe typhoons is significantly lower, and the mean intensity of TCs is prominently stronger; in La Nifia years, however, the opposite comes true. 相似文献
20.
基于CCMP风场的中国近海18个海区海面大风季节变化特征分析 总被引：3，自引：0，他引：3
利用1988-2010年CCMP(Cross Calibrated Multi-Platform)高时空分辨率10 m风场分析了我国近海海区的大风(6级以上)日数和大风风速的空间分布特征,并且按照中央气象台对近海海区的划分,分析了近海18个海区大风的季节变化特征.我国近海大风日数高值中心及大风风速高值中心都集中于巴士海峡、台湾海峡和南海东北部海域,在巴士海峡和南海东北部海域交界处最高可达140天以上,平均大风风速达到13m/s以上.从季节变化来看,大风日数和大风风速充分体现了东亚季风冬强夏弱的特点.冬半年,大风日数及风速高值中心一直位于东海东北部、台湾海峡、巴士海峡、南海东北部以及南海西南部海域,12月是一年之中大风日数和强度的峰值时期.从4月开始,南海西南部的高值中心消失,而以北海域的高值区的分布基本不变,这种情况一直持续到9月.近海18个海区的季节变化呈现出不同的区域差别,南海中部和南部的4个海域大风日数呈双峰型变化,冬季的12月至次年1月出现最高值,夏季西南季风时期的7-8月出现次高值.除琼州海峡外,包括南海北部海域的其余13个海区高值均在冬季12月至次年1月,低值出现在夏季6-7月. 相似文献