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1.
西北太平洋热带气旋源地变化特征及与局地海表温度的关系 总被引：2，自引：0，他引：2
为提高热带气旋的短期气候预测水平,利用1950-2005年西北太平洋热带气旋(TC)和表层水温(SST)资料,分析了西北太平洋TC生成位置分布的一般气候特征,季节、年际变化特征及其与局地SST之间的关系,同时还探讨了TC强度、路径与TC生成位置之间的关系.结果表明,西北太平洋存在4个TC高频源地,分别是南海中北部偏东洋面、菲律宾以东附近洋面、关岛附近洋面和马绍尔群岛附近洋面,其中关岛附近洋面TC发生数最多,是TC发生的一个主要源地.TC生成位置分布存在显著的季节和年际变化特征,这种变化与局地SST存在密切的关系,局地SST升高,TC生成位置偏西、偏北,反之,则偏东、偏南.同时发现,TC生成位置西北边界与月平均SST的27.5℃等温线具有较好的匹配关系,绝大多数TC都发生在月平均SST≥27.5℃的海区.TC强度、路径与TC生成位置之间存在一定的关系.TC生成位置偏东偏南,其发展强度相对较强,路径偏东偏南,可导致影响我国南部海区和日本东部沿海的TC个数增加;TC生成位置偏西偏北,其发展强度相对较弱,路径偏西北,可导致影响我国东部和北部沿海的TC个数增加. 相似文献
2.
西北太平洋热带气旋移动路径的年际变化及其机理研究 总被引：19，自引：3，他引：19
利用JTWC的热带气旋资料、NCEP/NCAR再分析的风场资料以及Scripps海洋研究所的海温资料分析了西北太平洋热带气旋(TC)移动路径的年际变化及其机理。结果表明,西北太平洋TC移动路径有明显的年际变化并与西太平洋暖池热状态有很密切的关系。当西太平洋暖池处于暖状态,西北太平洋上空TC移动路径偏西,影响中国的台风个数偏多;相反,当西太平洋暖池处于冷状态,西北太平洋的TC移动路径偏东,影响日本的台风个数偏多,而影响中国的台风个数可能偏少。本研究以西太平洋暖池处于冷状态的2004年与西太平洋暖池处于暖状态的2006年的西北太平洋TC移动路径的差别进一步论证了这一分析结果并从动力理论方面分析了在西太平洋暖池不同热状态下,季风槽对赤道西传天气尺度的Rossby重力混合波转变成热带低压型波动(TD型波动)的影响,以此揭示西太平洋暖池的热状态对西北太平洋TC生成位置与移动路径年际变化的影响机理。分析结果表明,当西北太平洋暖池处于暖状态时,季风槽偏西,使得热带太平洋上空对流层低层Rossby重力混合波转变成TD型波动的位置也偏西,从而造成TC生成平均位置偏西,并易于出现西行路径;相反,当西太平洋暖池处于冷状态时,季风槽偏东,这造成了对流层低层Rossby重力混合波转变成TD型波动的区域,以及TC生成的平均位置都偏东,从而导致TC移动路径以东北转向为主。 相似文献
3.
Relationship over southern China between the summer rainfall induced by tropical cyclones and that by monsoon 
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下载免费PDF全文 《大气和海洋科学快报》2017,(1)
本文分析华南夏季风降水(P_(SM))与热带气旋降水(P_(TC))在年际和年代际尺度上的物理联系,结果表明:在年际变化上,华南P_(SM)与P_(TC)呈显著负相关。南海-西北太平洋的气旋性涡度和相对湿度增加以及垂直风切变减弱,有利于更多的热带气旋生成,从而使得华南P_(TC)增加。同时异常增暖的赤道中太平洋SST和异常偏冷的北印度洋SST会激发南海-西太平洋异常气旋,加之中国东部-日本异常反气旋的作用,使得华南P_(SM)减少。在年代际尺度上,华南P_(SM)与P_(TC)呈显著正相关,在1990s初华南P_(SM)与P_(TC)明显增加。其中,南海生成的热带气旋对华南P_(TC)年代际增多有重要贡献。前期冬春季西太平洋持续异常偏暖的SST会通过垂直环流的作用引起热带印度洋SST增暖并持续到夏季,之后偏暖的热带印度洋SST又反馈作用于西北太平洋异常反气旋,使得华南P_(SM)增加。1990s初南海夏季风爆发年代际偏早,促使华南上空的大气显热源从5月持续增加至夏季,从而有助于东亚副热带夏季风的增强和华南P_(SM)增加。 相似文献
4.
赤道中东太平洋表层水温异常与热带气旋活动的统计关系 总被引：7，自引：4，他引：3
利用1950-2005年西北太平洋热带气旋(TC)和赤道中东太平洋表层水温(SST)资料,统计分析了赤道中东太平洋表层水温异常与TC频数、强度、源地和路径等的关系.结果表明,赤道中东太平洋暖异常年:(1)TC发生频数偏少,较常年平均偏少2～3个,但强度偏强,强台风和超强台风发生数偏多,较常年平均偏多1个左右,且随着暖异常强度的增强,TC发生频数偏少,强度增强愈加明显;(2)TC生成位置偏东偏南,145°E以东海区TC生成频数较冷异常年和La Nina年增加明显;(3)TC路径偏东,转向路径出现频次增加,西向路径出现频次减少,从而导致日本东部海区TC通过频数增加,而我国南海和华东沿海TC通过频数减少;(4)在我国登陆的TC频数偏少,较常年平均偏少1～2个.赤道中东太平洋冷异常年,情况基本与上相反.上述影响主要是由于赤道中东太平洋SST异常导致大气环流发生异常造成的. 相似文献
5.
GFDL_RegCM对21世纪西北太平洋热带气旋活动的情景预估 总被引：1，自引：0，他引：1
首先评估了GFDL模式对西北太平洋热带气旋(TC)环境热力及动力因子的模拟性能,再利用夏威夷大学国际太平洋研究中心高分辨率区域气候模式( IPRC-RegCM),进行降尺度研究西北太平洋TC活动特征,在此基础上预估21世纪全球变暖背景下(A1B)西北太平洋TC活动的主要特点.结果显示,在西北太平洋TC活动区,GFDL控制试验的海平面温度(SST)比ERSST偏低.与NCEP/NCAR再分析资料相比,GFDL模拟的1980-1999年大尺度环流平均场表现为:副高脊线平均位置近乎一致,西伸脊点偏东,强度偏弱,面积偏小;季风槽槽线的范围偏小,强度偏弱;水平风垂直切变值在南海及菲律宾群岛海域偏小,而在160°E～170°W的20°N以南偏强.与NCEP/NCAR强迫的模拟结果相比,GFDL强迫得到的TC源地频数在南海偏少,菲律宾群岛以东海域偏多,两者的季节及年际变化特征相似.路径频数在南海北部和我国华南沿岸显著偏多.AlB情景下,西北太平洋TC生成数目将增加一倍,生成源地偏北且同时向东部洋而扩展,路径频数增多主要发生在20°N以北的中东部洋面上,移经西北太平洋西部的TC频数减少,由此影响我国的TC将减少.TC频数的季节分布发生较大变化,最多的月份在10月.TC平均强度增强,最大强度在10月增加最多,这与10月SST的增加和环境风切变的减小均为最大值有密切的关系. 相似文献
6.
西北太平洋热带气旋强度变化的若干特征 总被引：2，自引：0，他引：2
使用NOAA海表温度资料、ECMWF再分析资料和JTWC台风最佳路径数据,对1984—2013年30年西北太平洋热带区域（100 °E~180 °,0~60 °N）内热带气旋（TC）的强度变化特征及其与环境风垂直切变（VWS）、海表温度（SST）、最大风速半径（RMW）的关系作了统计分析,尤其关注TC强度突变。结果表明:（1）在研究区域内,TC样本中35.2%强度稳定,52.8%强度变化缓慢,仅12.0%强度突变,约92.7%的迅速加强TC样本发生在其台风及以上强度等级;（2）2000年以来,TC强度稳定样本减少,强度迅速变化样本增多。5月和9—10月是TC强度突变的高频期;（3）超过12 m/s的环境VWS下TC迅速加强较少,且只有台风及以上强度TC才能在大于12 m/s的VWS下迅速加强;（4）TC加强和迅速加强主要在28.5~30.0 ℃的SST洋面上发生,在较低SST下仍迅速加强的TC强度等级较高;（5）TC样本的RMW多小于100 km,其中强度突变TC RMW峰值区在20~40 km;（6）加强TC的RMW的24 h变化一般减小,减弱TC的RMW则增大;其中强度突变TC尤其明显,超强台风发生迅速加强时,RMW减小的比率达84.6%,但仍有15.4%比率的RMW增大。 相似文献
7.
利用1979—2018年ERA Interim地面10 m风场、位势高度场、温度场和风场,Hadley中心HadISST再分析海温资料,采用SVD分析、合成分析等方法,研究了夏季（6—8月）西太平洋暖池关键海域海表面温度（Sea Surface Temperature,简称SST）对华东海域夏季10 m日最大风速变化的影响关系。SVD分析结果表明,夏季华东近海风速变化与菲律宾以东海域SST有明显负相关,第一模态左、右空间向量的时间系数相关达0.58,通过了置信度为95%的显著性检验。当西太平洋暖池SST正异常时,暖池海域SST增高,西北太平洋副热带高压（以下简称副高）加强,副高脊线北进（西北太平洋副高脊线纬度位置与暖池SST相关系数达到0.46,通过置信度为95%显著性检验）。此时华东近海正处于副高控制,近海下沉运动增强,大气温度垂直剖面有普遍增温现象,10 m风场有偏北风异常,海面风速减小约占40 a平均风速的约30%;当暖池SST负异常时,副高东撤南退,华东近海冷空气活动加强,温度垂直剖面存在显著降温现象,华东近海风速增加占40 a平均风速的20%以上。本研究进一步说明了暖池SST异常是一个有效的预报因子,可用于华东近海海面风速预测预报。 相似文献
8.
20世纪印度洋气候变率特征 总被引：28，自引：3，他引：28
利用时间连续性相对较为理想的 GISST资料 ,分析了 2 0世纪印度洋气候变率的基本特征 ,探讨了它与赤道中、东太平洋和西太平洋暖池区气候变化之间的联系 ,结果表明 :(1 )北印度洋 SST的季节变化具有鲜明的季风特征 ,在西南季风爆发期 ,海温达到全年最冷 ;南印度洋 SST的季节循环特征较为合乎常规 ,大致落后太阳辐射季节循环 2个月左右 ;赤道印度洋沿着非洲东海岸 ,SST的季节变化受季风带影响显著 ,但在赤道中东印度洋 ,SST的季节循环特征不明显。(2 )印度洋 ,特别是 2 0°S以北的热带印度洋 SST的变化 ,具有显著的整体一致性 ,自 2 0世纪 50年代中期以来持续变暖 ,赤道印度洋增暖了大约 0 .6℃。当赤道中东太平洋出现暖异常时 ,2 0°S以北的热带印度洋海域同样出现暖异常 ;赤道印度洋 SST与 Nino3区指数的相关系数 ,在滞后 Nino 3区指数 4～ 5个月左右达到最大。 (3)西太平洋暖池区 SST的变化 ,与南印度洋西风漂流区、赤道北印度洋存在显著的正相关。在年代际的时间尺度上 ,赤道印度洋和西太平洋暖池区 SST的变率特征极为一致。 (4)南印度洋 SST的年际振荡幅度 ,远强于热带印度洋 ;南印度洋的 SST演变特征 ,从统计上看 ,更多地与西太平洋暖池 SST变化相协调。 相似文献
9.
热带太平洋和印度洋海温年际变化的均方差分析 总被引：5，自引：0，他引：5
运用1951～1997年热带（20°N～20°S,50°E～80°W）海温（SST）资料求出其各月的均方差,结果表明:太平洋海温变化相对印度洋海温变化要明显,特别是赤道中东太平洋附近 （165～90°W,6°N～6°S）的海温变化比较显著,其海温的变化范围在2～4°C左右,3～4月份海温年际变化小,11～12月海温年际变化大;“暖池”附近洋面海温年际变化也小。而印度洋海域的海温变化范围在1～2°C左右,在印度洋南半球洋面海温变化比北半球洋面海温变化相对较大。同时,根据上述海温变化特征确定了几个海温年际变化最大的关键区。 相似文献
10.
为探索赤道西太平洋暖池次表层水温异常与热带气旋的关系,用赤道西太平洋暖池和南海SOTA实测资料,对TC的影响做了统计分析。赤道西太平洋暖池SOTA与同步西太平洋TC个数不存在线性相关;赤道西太平洋暖池1月SOTA滞后5～7个月影响西太平洋的TC;赤道西太平洋暖池区1月的SOTA出现正(负)距平值时,当年西北太平洋和南海的TC生成时间比常年提早(推迟)是主要现象,极值年份尤其明显,当年夏季西北太平洋副热带高压偏弱(强),位置偏北(南),西太平洋暖池区上空对流加强(减弱),对台风生成有(不)利,台风生成平均位置偏西(东),TC的个数偏多(少)、偏强(弱),易于出现西行(东北转向)路径为主;南海中北部2月SOTA出现偏暖(冷)年,当年南海TC生成日期偏早(晚)、数量偏多(少)、偏强(弱)是主要现象。赤道西太平洋暖池SOTA对TC影响明显,时间滞后。 相似文献
11.
The Dynamic and Thermodynamic Effects of Relative and Absolute Sea Surface Temperature on Tropical Cyclone Intensity 总被引：1，自引：0，他引：1 下载免费PDF全文
下载免费PDF全文 Several numerical experiments were performed to investigate the dynamic and thermodynamic effects of sea surface temperature(SST) on tropical cyclone(TC) intensity.The results reveal that the relative SST within a radius of 2-3 times the radius of maximum wind contributes positively and greatly to TC intensity,while the remote SST far away from the TC center could reduce storm intensity.The change of air-sea temperature and moisture differences may be the reason why TC intensity is more sensitive to the relative rather than the absolute SST.As the inflow air moves toward the eyewall,warmer(colder) remote SST can gradually increase(decrease) the underlying surface air temperature and moisture,and thus decrease(increase) the air-sea temperature and moisture differences,which lead to less(more) energy fluxes entering the eyewall and then decrease(increase) the TC intensity and make it less sensitive to the absolute SST change.Finally,with all the related dynamic and thermodynamic processes being taken into account,a schematic diagram for the effects of relative SST and absolute SST on TC intensity is proposed. 相似文献
12.
The power dissipation index (PDI), which is defined as the sum of the cube of tropical cyclone (TC) maximum wind speed during TC lifetime, is widely used to estimate the TC destructive potential. However, due to the lack of high-resolution observations, little attention has been paid to the contribution of TC size change to TC destructive potential in response to ocean warming. In this study, sensitivity experiments are performed by using the high-resolution Weather Research and Forecasting (WRF) model to investigate the responses of TC size and TC destructive potential to prescribed sea surface temperature (SST) increase under the present climate condition. The results show that TC size increases with the ocean warming. Possible reasons for TC size change are investigated with a focus on the outer air-sea moisture difference (ASMD). As SST increases, ASMD in the outer zone of the TC is larger than that in the inner zone, which increases the surface entropy flux (SEF) of the outer zone. This change in the radial distribution of SEF causes the increase of tangential wind in the outer zone, which further increases SEF, resulting in a positive feedback between outer-zone SEF and outer-zone tangential wind. This feedback leads to the increase of the radius of gale-force wind, leading to the expansion of TC size. Moreover, to estimate the contribution of TC size change to TC destructiveness, we calculate TC size-dependent destructive potential (PDS) as the storm size information is available in the model outputs, as well as PDI that does not consider the effect of TC size change. We find that PDS increases exponentially as SST increases from 1 to 4°C, while PDI increases linearly; hence the former is soon much greater than the latter. This suggests that the growth effect of TC size cannot be ignored in estimating destructiveness under ocean warming. 相似文献
13.
A 2-km resolution simulation using the Weather Research and Forecasting model with Morrison microphysics was employed to investigate the rainwater microphysical properties during different stages of Typhoon Usagi(2013) in the inner-core and outer region. The model reproduced the track, intensity, and overall structure of Usagi(2013) reasonably. The simulated raindrop size distribution showed a rapid increase in small-size raindrop concentration but an oscillated decrease in large-size ones in the inner-core region, corresponding well with the upward motion. It was found that there existed two levels(1.25 and 5.25 km) of maximum number concentration of raindrops. The ice-related microphysics at high levels was stronger than the warm-rain processes at low levels. The larger raindrops formed by self-collection in the inner-core suffered from significant breakup, but the raindrops outside the eyewall did not experience evident breakup. Model results indicated that the dominant terms in the water vapor budget were the horizontal moisture flux convergence(HFC) and local condensation and deposition. The evaporation from the ocean surface(PBL) was ~10% of the HFC in the inner core, but up to 40% in the outer region as the air therein was far from saturation. Furthermore, water vapor in the outer region was obtained equally through evaporation from the cloud and inward transportation from the environment. An earlier start of cloud microphysical processes in the inner-core region was evident during the intensification stage, and the continuous decreasing of condensation in both the inner-core and outer regions might imply the beginning of the storm weakening. 相似文献
14.
特大眼台风Winnie（1997）的高分辨率数 值模拟 总被引：2，自引：1，他引：2
台风Winnie 1997的眼直径为370 km,是有观测以来发现的最大台风眼之一。应用Penn State/NCAR高分辨率中尺度模式MM5,成功地模拟了Winnie的路径、强度、台风眼及其双眼壁结构。由此根据模式输出结果分析了台风眼及内外眼壁附近的流场和热力场特征。发现Winnie台风的眼壁及其周围风场都显示了明显的非对称性结构。Winnie的外眼壁对应一个极大风速环,也是暖湿环和正涡度环。内眼壁对应一个次极大风速环、暖湿环。上升运动控制整个内眼壁和海平面2 km以上的外眼壁区域,下沉运动则控制眼区和内外眼壁之间。径向入流集中在外眼壁和内外眼壁之间的边界层,流出则位于外眼壁的对流层中上层。 相似文献
15.
The sensitivity of the simulation of tropical cyclone(TC) size to microphysics schemes is studied using the Advanced Hurricane Weather Research and Forecasting Model(WRF). Six TCs during the 2013 western North Pacific typhoon season and three mainstream microphysics schemes–Ferrier(FER), WRF Single-Moment 5-class(WSM5) and WRF Single-Moment6-class(WSM6)–are investigated. The results consistently show that the simulated TC track is not sensitive to the choice of microphysics scheme in the early simulation, especially in the open ocean. However, the sensitivity is much greater for TC intensity and inner-core size. The TC intensity and size simulated using the WSM5 and WSM6 schemes are respectively higher and larger than those using the FER scheme in general, which likely results from more diabatic heating being generated outside the eyewall in rainbands. More diabatic heating in rainbands gives higher inflow in the lower troposphere and higher outflow in the upper troposphere, with higher upward motion outside the eyewall. The lower-tropospheric inflow would transport absolute angular momentum inward to spin up tangential wind predominantly near the eyewall, leading to the increment in TC intensity and size(the inner-core size, especially). In addition, the inclusion of graupel microphysics processes(as in WSM6) may not have a significant impact on the simulation of TC track, intensity and size. 相似文献
16.
热带气旋眼墙非对称结构的研究综述 总被引：2，自引：0，他引：2
热带气旋的眼墙非对称结构与其发展过程密切相关。在热带气旋移动过程中,非对称风场伴随着边界层内非对称摩擦而引起的辐合,影响着热带气旋眼墙内的对流分布。此外,风垂直切变作为影响热带气旋强度的重要因子,将上层暖心吹离表层环流,引起眼墙垂直运动的非对称,导致云、降水在方位角方向的非均匀分布。当存在平均涡度的径向梯度时,罗斯贝类型的波动可以存在于涡旋内核区域,影响眼墙非对称结构。海洋为热带气旋提供潜热和感热形式的能量,是热带气旋发展的重要能量来源,关于海洋如何影响热带气旋眼墙非对称结构的相关研究较少。文中着重回顾了热带气旋与海洋相互作用的研究成果,并提出海洋影响热带气旋眼墙非对称结构的机制。海洋对热带气旋最显著的响应特征是冷尾效应,该效应通过降低海表温度,减少海洋向大气输送的潜热和感热,从而影响热带气旋眼墙非对称结构。此外,海浪改变海表粗糙度,通过边界层影响移动热带气旋的眼墙结构。 相似文献
17.
Recent studies found that in the context of global warming, the observed tropical cyclones (TCs) exhibit significant poleward migration trend in terms of the mean latitude where TCs reach their lifetime-maximum intensity in the western North Pacific (WNP). This poleward migration of TC tracks can be attributed to not only anthropogenic forcing (e.g., continuous increase of sea surface temperature (SST)), but also impacts of other factors (e.g., natural variability). In the present study, to eliminate the impacts of other factors and thus focus on the impact of unvaried SST on climatological WNP TC tracks, the mesoscale Weather Research and Forecasting (WRF) model is used to conduct a suite of idealized sensitivity experiments with increased SST. Comparisons among the results of these experiments show the possible changes in climatological TC track, TC track density, and types of TC track in the context of SST increase. The results demonstrate that under the warmer SST conditions, the climatological mean TC track systematically shifts poleward significantly in the WNP, which is consistent with the previous studies. Meanwhile, the ocean warming also leads to the decreased (increased) destructive potential of TCs in low (middle) latitudes, and thus northward migration of the region where TCs have the largest impact. Further results imply the possibility that under the ocean warming, the percentage of TCs with westward/northwestward tracks decreases/increases distinctly. 相似文献
18.
利用TMI反演的水汽凝结物对热带气旋潜热结构分布的探索研究 总被引：3，自引：0，他引：3
本文利用热带测雨卫星TRMM（Tropical Rainfall Measuring Mission）微波成像仪TMI（TRMM Microwave Imager）2A12 水汽凝结物（Hydrometeor）反演资料,对西北太平洋地区从1998～2009 年的236 个热带气旋个例的1776 个“快照”（snapshot）的水汽凝结物的结构特征进行了分析,并探讨了水汽凝结物的时空变化与热带气旋强度演变联系。研究结果表明:（1）TMI 2A12 水汽凝结物资料显示出了热带气旋内部的细致结构及变化特征,水汽凝结物的峰值集中于数十公里到一百多公里的热带气旋眼壁及云墙区;在热带气旋发展过程中,随着热带气旋强度的增强,水汽凝结物增多且往其中心靠拢,从发展阶段到成熟阶段,水汽凝结物的大值中心基本上集中在距离热带气旋中心约50 km 区域,而且强度越强的热带气旋,水汽凝结物的大值中心与热带气旋中心的距离越近;在热带气旋消亡的过程中,水汽凝结物不断减弱且往外围扩散,逐渐扩展到远离中心的区域;（2）热带气旋强度与水汽凝结物的分布关系密切,热带气旋强度变化与热带气旋中心附近200 km 范围内的水汽凝结物含量存在显著的正相关,而200 km 以外的外围水汽凝结物含量存在负相关;（3）热带气旋强度变化与水汽凝结物的变化存在时间差,水汽凝结物的变化超前于热带气旋强度的变化,在热带气旋迅速发展之前数小时,热带气旋中心0～50 km 环状区域的水汽凝结物含量就已经提前增加了,在热带气旋减弱前数小时到十数小时,即使热带气旋还处于它强度的鼎盛时期,其中心0～50 km 环状区域的水汽凝结物含量就已经提前显著减少了,这种水汽凝结物的变化超前于热带气旋强度的变化的现象,可能是热带气旋强度预报的潜在线索。 相似文献
19.
Typhoon Winnie (1997) was one of the hurricanes that had extremely large eyewall ever recorded with a diameter of eyewall reaching 370 km. Using the Penn State University/National Center for Atmospheric Research mesoscale model MM5 with 3-km grid horizontal spacing on the finest nested mesh, Winnie was successfully simulated in terms of track, intensity, eye and concentric eyewalls. The dynamic and thermal structures of concentric eyewalls were studied based on the model output. It was found that the concentric eyewalls and their surrounding wind fields were asymmetric in observation as well as in simulation. Winnie's outer eyewall was associated with a maximum wind ring, a warm moist ring, and a high vorticity ring. The inner eyewall was associated with a secondary maximum wind ring and a warm moist ring. Upward motion dominated the whole layer of inner eyewall and the area above 2-km altitude of the outer eyewall. Downward motion was found inside the eye and the moat. Radial inflow happened in the boundary layer of the outer eyewall and the moat, but radial outflow dominated the middle and upper levels of the outer eyewall. 相似文献
20.
Based on high-fidelity numerical simulation by using the Weather Research and Forecast (WRF) model, we analyzed the formation and replacement mechanism of the concentric eyewall of Super Typhoon Muifa (1109) from the aspects of the potential vorticity (PV), dynamic/ thermodynamic structure change, sea surface flux, and water vapor content. Observational data and sensitivity tests were also adopted to verify the results. We found that: (1) The abnormal increase of the PV in the rain zone is mainly due to the condensation latent heat. Sufficient water vapor conditions are beneficial to the formation of the outer eyewall structure, and when the environmental water vapor content is larger, the intensity of the outer eyewall becomes greater. (2) After the formation of the typhoon’s outer eyewall, in the area where the outer eyewall is located, the increase of inertial stability contributes to the decrease of the intensity of the inner eyewall. When the intensity of the outer eyewall is larger, the divergence and subsidence motion in the upper layer of the outer eyewall has a greater weakening effect on the intensity of the inner eyewall. (3) The increase of potential temperature of the outer eyewall is mainly due to the condensation latent heat release and the warming of dry air subsidence motion in the moat area. (4) The increase of sea surface heat flux can prolong the concentric eyewall replacement process. 相似文献