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Frontogenesis and frontolysis of cold filament impacted by different directions of wind and wave fields using large eddy simulation
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作者 Guojing LI Dongxiao WANG +2 位作者 Changming DONG Yeqiang SHU Yunkai HE 《Journal of Oceanology and Limnology》 2025年第3期676-691,共16页
The variations of the frontogenetic activity of cold filament driven by the different angle(θ=0°,22.5°,45°,67.5°,and 90°)of the wind and wave fields and the filament axis are studied by non h... The variations of the frontogenetic activity of cold filament driven by the different angle(θ=0°,22.5°,45°,67.5°,and 90°)of the wind and wave fields and the filament axis are studied by non hydrostatic large eddy simulation.Conversion between the frontogenesis and frontolysis of cold filament were created by the chang in the direction of secondary circulations.The changes in the direction of secondary circulation are induced by the Coriolis Effect regardless of wind direction and wave fields.The destructive action of the wind and wave fields on symmetry of the submesoscale flow fields becomes weak as the angle increases.The secondary downwelling jet induced by Stokes shear force is gradually close to that associated with secondary circulations as the angle changes fromθ=0°to 45°and then the downwelling jet is only created by secondary circulations forθ=67.5°and 90°.The frontogenetic intensity of cold filament may be impacted by the angle of the wind and wave fields and the filament axis.The reason is that firstly the odd-symmetry of secondary circulations enhances with the angle increasing,and secondary the secondary downwelling jet created the Stokes shear force gradually weakens and then disappears with the angle increasing. 展开更多
关键词 cold filament frontogenesis FRONTOLYSIS secondary circulation
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A Generalized Frontogenesis Function and Its Application 被引量:16
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作者 YANG Shuai GAO Shouting LU Chungu 《Advances in Atmospheric Sciences》 SCIE CAS CSCD 2014年第5期1065-1078,共14页
With the definition of generalized potential temperature, a new generalized frontogenesis function, which is expressed as the Lagrangian change rate of the magnitude of the horizontal generalized potential temperature... With the definition of generalized potential temperature, a new generalized frontogenesis function, which is expressed as the Lagrangian change rate of the magnitude of the horizontal generalized potential temperature gradient, is derived. Such a frontogenesis function is more appropriate for a real moist atmosphere because it can reflect frontogenesis processes, in which the atmosphere in a frontal zone is typically characterized by neither completely dry nor uniform saturation. Furthermore, by derivation, the expression of generalized frontogenesis function includes both temperature and humidity gradients, which is different from and superior to the traditional frontogenesis function in moist processes, which also uses equivalent potential temperature. Diagnostic studies of real cases are performed and show that the generalized frontogenesis function in non- uniformly saturated moist atmosphere indeed provides a useful tool for frontogenesis, compared to using the traditional frontogenesis function. The new frontogenesis function can be used in situations involving either a strong temperature or moisture gradient and is closely correlated with precipitation. 展开更多
关键词 frontogenesis diagnostic analysis case study
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Investigation of the Mei-yu Front Using a New Deformation Frontogenesis Function 被引量:10
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作者 YANG Shuai GAO Shouting Chungu LU 《Advances in Atmospheric Sciences》 SCIE CAS CSCD 2015年第5期635-647,共13页
A new frontogenesis function is developed and analyzed on the basis of a local change rate of the absolute horizontal gradient of the resultant deformation. Different from the traditional frontogenesis function, the n... A new frontogenesis function is developed and analyzed on the basis of a local change rate of the absolute horizontal gradient of the resultant deformation. Different from the traditional frontogenesis function, the newly defined deformation frontogenesis is derived from the viewpoint of dynamics rather than thermodynamics. Thus, it is more intuitive for the study of frontogenesis because the compaction of isolines of both temperature and moisture can be directly induced by the change of a flow field. This new frontogenesis function is particularly useful for studying the mei-yu front in China because mei-yu rainbands typically consist of a much stronger moisture gradient than temperature gradient, and involve large deformation flow. An analysis of real mei-yu frontal rainfall events indicates that the deformation frontogenesis function works remarkably well, producing a clearer mei-yu front than the traditional frontogenesis function based on a measure of the potential temperature gradient. More importantly, the deformation frontogenesis shows close correlation with the subsequent(6 h later) precipitation pattern and covers the rainband well, bearing significance for the prognosis or even prediction of future precipitation. 展开更多
关键词 DEFORMATION frontogenesis PRECIPITATION
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Evolution and Frontogenesis of an Imbalanced Flow- the Influence of Vapor Distribution and Orographic Forcing 被引量:6
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作者 王云峰 伍荣生 潘益农 《Advances in Atmospheric Sciences》 SCIE CAS CSCD 2000年第2期256-274,共19页
If the initial fields are not in geostrophic balance, the adjustment and evolution will occur in the stratified fluid. and the frontogenesis will occur under suitable conditions. The evolution is studied here with a n... If the initial fields are not in geostrophic balance, the adjustment and evolution will occur in the stratified fluid. and the frontogenesis will occur under suitable conditions. The evolution is studied here with a nonhydrostatic fully compressible meso-scale model (Advanced Regional Prediction System, ARPS). Four cases are designed and compared: (i) control experiment: (ii) with different initial temperature gradient; (iii) with vapor distribution; (iv) with orographic forcing. The results show that: (1) there is an inertial oscillation in the evolution of the imbalanced flow with the frequency of the local Coriolis f, and with its amplitude decreasing with time. The stationary balanced state can only be approached as it cannot be reached in the limit duration of time. The energy conversion ratio varies in the range of [0, 1; 3]; (2) the stronger initial temperature gradient can make the final energy conversion ratio higher. and vice versa; (3) suitable vapor distribution is favorable for the frontogenesis. It will bring forward the time of the frontogenesis, strengthen the intensity of the cold front, and influence the final energy conversion ratio; (4) the orographic forcing has an evidently strengthening effect on the frontogenesis. The strengthening effect on the frontogenesis and the influence on the final energy conversion ratio depend on the relative location of the mountain to the cold front. 展开更多
关键词 EVOLUTION frontogenesis inertial oscillation vapor distribution and orographic forcing
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Topographic Effect on Geostrophic Adjustment and Frontogenesis 被引量:5
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作者 方娟 伍荣生 《Advances in Atmospheric Sciences》 SCIE CAS CSCD 2001年第4期524-538,共15页
Three conservative principles: potential vorticity, absolute momentum and potential temperature are used to study the influence of topography on the local frontogenesis and geostrophic adjustment, which are induced by... Three conservative principles: potential vorticity, absolute momentum and potential temperature are used to study the influence of topography on the local frontogenesis and geostrophic adjustment, which are induced by the inhomogeneous thermal fields. It is found that the horizontal distribution of the initial potential temperature and its position relative to the mountain play important roles during the geostrophic adjustment and local frontogenesis. The frontogenesis is weakened by the mountain when the initial thermal perturbation is located at the base of the upwind slope. The frontal discontinuity cannot occur unless the horizontal contrast of the initial potential temperature is great enough. Whereas, the situation is opposite when the initial thermal disturbance is main-ly situated near the peak of the mountain. Complementary to the aforementioned cases, the effect of topog-raphy on the frontogenesis depends on the stratification of the flow when the initial thermal disturbance lies at the foot of lee slope. For weak stratification, topography is favorable to the formation of frontal discontinuity, vice versa. This discrepancy is attributed to the difference of subsidence warming, caused by the mountain, when the stratification is either strong or weak. Furthermore, the energy conversion ratio between the kinetic and potential energy during the geostrophic adjustment process is also affected by the topography. In contrast to the flat bottom case, the ratio is reduced (increased) when the initial thermal perturbation lies in the up-wind slope (lee slope). The reason is that the gravity force does negative work in the former case while does positive work in the latter case. Key words Topography - Geostrophic adjustment - Frontogenesis This work was supported by the National Natural Science Foundation of China under Grant 49735180, and by the State Key Basic Program: CHERES. 展开更多
关键词 TOPOGRAPHY Geostrophic adjustment frontogenesis
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Interaction of Diabatic Frontogenesis and MoistureProcesses in Cold-Frontal Rain-Band 被引量:3
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作者 王春明 伍荣生 王元 《Advances in Atmospheric Sciences》 SCIE CAS CSCD 2002年第3期544-561,共18页
Three-dimensional simulation of cold-front rain-band (NCFR) associated with a straight cold front has been studied by use of a non-hydrostatic, full compressible storm-scale model (ARPS) including multi-phase microphy... Three-dimensional simulation of cold-front rain-band (NCFR) associated with a straight cold front has been studied by use of a non-hydrostatic, full compressible storm-scale model (ARPS) including multi-phase microphysical parameterization. The dynamical and physical features of the frontal cloud de-velopment have been well simulated and analyzed. It is in evidence that the frontal cloud is triggered by the updraft of the secondary frontal circulation. However, the long persistence of diabatic frontogenesis only can be attributed to positive feedback between the frontal baroclinicity and the prefrontal latent heat release. The simulations indeed demonstrate that the potential temperature gradient enhancement in front zone is strongly related with the re-distribution of cloud moisture, by the action of tilted updraft. In conse-quence, the splice of cooling and heating pool that is respectively created from the evaporation of cloud wat-er and condensing J freezing of water vapor J rain droplet, wich is in favor of the strong contrast of cool and warm air mass across the frontal zone to diabatic frontogenesis. 展开更多
关键词 NCFR Diabatic frontogenesis Moisture heating FEEDBACK
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Mechanism of Balanced Flow and Frontogenesis 被引量:3
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作者 伍荣生 方娟 《Advances in Atmospheric Sciences》 SCIE CAS CSCD 2001年第3期323-334,共12页
The final balanced state of an initial unbalanced flow is discussed with the same method as Vallis (1992). For the two-dimensional, inviscid, rotating and nonlinear model, the final state of the flow depends on the in... The final balanced state of an initial unbalanced flow is discussed with the same method as Vallis (1992). For the two-dimensional, inviscid, rotating and nonlinear model, the final state of the flow depends on the initial conditions. If the initial potential vortcity of the flow is non-uniform, the final state is not necessarily geostrophic. However, for the zero and uniform potential vorticity flow, the final state will satisfy the thermal wind relation when the length scale of the initial disturbance is large enough. Otherwise, discontinuity will occur in the geostrophic solution. In this case, the final balanced state will not be geostrophic any longer and an extended momentum coordinate is introduced to overcome the mult-value problem. Key words Frontogenesis - Geostrophic adjustment - Thermal wind balance - Extended momentum coordinates The work was supported by the National Natural Science Foundation of China (Grant Nos. 49735180 and 40075011) and the State Key Basic Program: CHERES. 展开更多
关键词 frontogenesis Geostrophic adjustment Thermal wind balance Extended momentum coordinates
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Frontogenesis,Evolution and the Time Scale of Front Formation 被引量:1
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作者 方娟 伍荣生 《Advances in Atmospheric Sciences》 SCIE CAS CSCD 1998年第2期100-113,共14页
Observational study shows that, in some cases, the frontal structure displays the features of gravitative flows. It seems that the formation of discontinuity is an important problem in the study of the frontogenesis w... Observational study shows that, in some cases, the frontal structure displays the features of gravitative flows. It seems that the formation of discontinuity is an important problem in the study of the frontogenesis which is usually defined as an increasing of the scalar gradient. In this paper, the characteristic features of air flow with initial imbalance between the wind and the density fields are studied. Much attention is paid on the condition for the formation of discontinuity and its time scale. It is found that the initial distribution of density plays an important role in the formation of the discontinuity which happens in short time duration. 展开更多
关键词 FRONT frontogenesis EVOLUTION Time scale
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Frontogenesis and Frontolysis of a Cold Filament Driven by the Cross-Filament Wind and Wave Fields Simulated by a Large Eddy Simulation 被引量:1
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作者 Guojing LI Dongxiao WANG +3 位作者 Changming DONG Jiayi PAN Yeqiang SHU Zhenqiu ZHANG 《Advances in Atmospheric Sciences》 SCIE CAS CSCD 2024年第3期509-528,共20页
The variations of the frontogenetic trend of a cold filament induced by the cross-filament wind and wave fields are studied by a non-hydrostatic large eddy simulation. Five cases with different strengths of wind and w... The variations of the frontogenetic trend of a cold filament induced by the cross-filament wind and wave fields are studied by a non-hydrostatic large eddy simulation. Five cases with different strengths of wind and wave fields are studied.The results show that the intense wind and wave fields further break the symmetries of submesoscale flow fields and suppress the levels of filament frontogenesis. The changes of secondary circulation directions—that is, the conversion between the convergence and divergence of the surface cross-filament currents with the downwelling and upwelling jets in the filament center—are associated with the inertial oscillation. The filament frontogenesis and frontolysis caused by the changes of secondary circulation directions may periodically sharpen and smooth the gradient of submesoscale flow fields.The lifecycle of the cold filament may include multiple stages of filament frontogenesis and frontolysis. 展开更多
关键词 cold filament frontogenesis FRONTOLYSIS large eddy simulation
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Application of the Artificial Compression Method to the Simulation of Two-Dimensional Frontogenesis
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作者 杨宏伟 王斌 季仲贞 《Advances in Atmospheric Sciences》 SCIE CAS CSCD 2002年第5期863-869,共7页
The artificial compression method (ACM) that is generally used to capture the contact discontinuity in nonviscous flows is used here in the simulation of quasi-geostrophic ideal frontogenesis in two dimensions. A comp... The artificial compression method (ACM) that is generally used to capture the contact discontinuity in nonviscous flows is used here in the simulation of quasi-geostrophic ideal frontogenesis in two dimensions. A comparison is made among the result of the ACM, the simulation result of Cullen, and the exact solution of the semi-geostrophic equations. The simulated front in this paper is more prominent than Cullen&#8242;s and is much closer to the exact solution. 展开更多
关键词 artificial compression method frontogenesis QUASI-GEOSTROPHIC semi-geostrophic
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Cold filament frontogenesis and frontolysis induced by thermal convection turbulence using large eddy simulation
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作者 Zewen Wu Guojing Li +1 位作者 Yunkai He Jintuan Zhang 《Acta Oceanologica Sinica》 SCIE CAS CSCD 2024年第9期26-34,共9页
The frontogenetic processes of a submesoscale cold filament driven by the thermal convection turbulence are studied by a non-hydrostatic large eddy simulation.The results show that the periodic changes in the directio... The frontogenetic processes of a submesoscale cold filament driven by the thermal convection turbulence are studied by a non-hydrostatic large eddy simulation.The results show that the periodic changes in the direction of the cross-filament secondary circulations are induced by the inertial oscillation.The change in the direction of the secondary circulations induces the enhancement and reduction of the horizontal temperature gradient during the former and later inertial period,which indicates that the frontogenetical processes of the cold filament include both of frontogenesis and frontolysis.The structure of the cold filament may be broken and restored by frontogenesis and frontolysis,respectively.The magnitude of the down-filament currents has a periodic variation,while its direction is unchanged with time.The coupling effect of the turbulent mixing and the frontogenesis and frontolysis gradually weakens the temperature gradient of the cold filament with time,which reduces frontogenetical intensity and enlarges the width of cold filament. 展开更多
关键词 cold filament frontogenesis FRONTOLYSIS thermal convection turbulence large eddy simulation
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Interaction of Mesoscale Convection and Frontogenesis
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作者 彭加毅 方娟 伍荣生 《Advances in Atmospheric Sciences》 SCIE CAS CSCD 2004年第5期814-823,共10页
On the basis of the MM5 simulation data of the severe storm that occurred over the southeastern part of Hubei province on 21 July 1998, the interaction of mesoscale convection and frontogenesis is dealt with using t... On the basis of the MM5 simulation data of the severe storm that occurred over the southeastern part of Hubei province on 21 July 1998, the interaction of mesoscale convection and frontogenesis is dealt with using the thermodynamical equation and frontogenetical function. The results show that the outbreak of the severe storm is closely related to the local frontogenesis. In fact, the interaction between the shearing instability of the low-level jet (LLJ) and the topographic forcing generates an gravity-inertia wave as well as local frontogenesis (the ?rst front), which consequently induce the onset of the severe storm. From then on, owing to the horizontal and vertical advection of the potential temperature, the new frontogenesis (the second front) is formed to the northeast side of the severe storm, which initiates the second rain belt. Meanwhile, a two-front structure emerges over the southeastern part of Hubei province. Accompanied with the further intensi?cation of the convection, the rain droplets evaporation cooling strengthens the ?rst front and weakens the second front, resulting in single front structure over the southeastern part of Hubei province in the period of the strong convection. 展开更多
关键词 mesoscale convection frontogenesis two-front structure
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A Numerical Study of Geostrophic Adjustment and Frontogenesis
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作者 伍荣生 《Advances in Atmospheric Sciences》 SCIE CAS CSCD 1998年第2期46-59,共14页
Using the PSU/NCAR Mesoscale Model version four(MM4), the frontogenesis and geostrophic adjustment problem in atmosphere with imbalance initial ideal data and conditions are studied. Based on results of experiments,... Using the PSU/NCAR Mesoscale Model version four(MM4), the frontogenesis and geostrophic adjustment problem in atmosphere with imbalance initial ideal data and conditions are studied. Based on results of experiments, it is found that the objective analysis and initialization procedure of the Model are not sensitive to the initial conditions used in this study. The final state of atmosphere, through process of adjustment, depends on the temperature gradient intensity of initial imbalance conditions. The front can be formed with appropriate condition. The processes of the frontogenesis are studied. It is also found that the response of the model to the ideal initial data used in this investigation is sensitive to the selected lateral boundary condition. The time-dependent inflow/outflow lateral boundary condition is the best implemented option for this numerical study. Energetic study of the experiments shows that the front is formed after the initial transient stage when there is no exchange of energy between the kinetic and potential energy. The time needed for the formation of the front is longer than that predicted theoretically. The ratio of kinetic energy to the released potential energy is considered. This ratio varies with the temperature gradient intensity and the type of used wind for computing kinetic energy (geostrophic or geostrophic plus ageostrophic wind). The larger temperature gradient, the larger magnitude of this ratio. A maximum value of energy in either type of computed kinetic energies (geostrophic wind kinetic energy and actual wind kinetic energy) for cases that the fronts are observed whereby, and its magnitude and occurrence time depend on initial data distribution. The variation of the computed kinetic energies with time, after transition time, is reasonable and no significant conversion of the energy between kinetic and potential energy goes on, however, stability within variables is not achieved. 展开更多
关键词 frontogenesis Geostrophic adjustment Energetics of geostrophic adjustment
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DIAGNOSIS OF THE DEVELOPMENTAL MECHANISM OF THE EXTRATROPICAL TRANSITION OF A TROPICAL CYCLONE USING POTENTIAL VORTICITY INVERSION OF FRONTOGENESIS
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作者 周毅 肖坤 宋辉 《Journal of Tropical Meteorology》 SCIE 2012年第3期360-368,共9页
This paper diagnoses and analyses the developmental mechanism of a process of extratropical transition of a tropical cyclone which occurred over West Pacific Ocean based on a diagnosis method of potential vorticity in... This paper diagnoses and analyses the developmental mechanism of a process of extratropical transition of a tropical cyclone which occurred over West Pacific Ocean based on a diagnosis method of potential vorticity inversion of frontogenesis.The study diagnoses quantitatively the role and effect of dynamic influence of westerly cold troughs,middle-latitude baroclinic frontal zones,cyclone cycles and unbalanced wind fields during the different stages of the extratropical transition of a tropical cyclone,and also discusses the interaction between them and the developmental mechanism.The results show that there are different developmental mechanisms during each stage of the extratropical transition and the processes are also unbalanced. 展开更多
关键词 extratropical transition of tropical cyclones frontogenesis potential vorticity mechanism analysis
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Numerical test of coastal frontogenesis
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作者 Shen Shaohua and Zhou Mingyu 《Acta Oceanologica Sinica》 SCIE CAS CSCD 1994年第1期57-72,共16页
A two-dimensional mesoscale model is used to investigate the effect of background wind field andcharacter of the underlying surface on the coastal frontogenesis along the east continental coast when cold air outbreak.... A two-dimensional mesoscale model is used to investigate the effect of background wind field andcharacter of the underlying surface on the coastal frontogenesis along the east continental coast when cold air outbreak. The results of numerical experiments indicate that the coastal frontogenesis mainly appears near ground atnight. When the background wind is easterly, it is favorable to coastal frontogenesis in the lower layer of the atmosphere. When the background wind is westerly, it is unfavorable to coastal frontogenesis in the lower layer of theatmosphere. The vertical shear of the background wind has important influence on the coastal frontogenesis. Thecoastal frontogenesis at lower layer at night is strengthened with increasing temperature difference between sea andair. The effect of coastal sloping terrain on the coastal frontogenesis is little when the topography sloping angle islesser.The analysis of the physical mechanism of frontogenesis shows that the main factor influencing the coastalfrontogenesis is the deformation field of horizontal wind speed. 展开更多
关键词 TEST Numerical test of coastal frontogenesis
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Linear Momentum Approximation and Frontogenesis Caused by Baroclinic Ekman Momentum Flow
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作者 何建中 《Advances in Atmospheric Sciences》 SCIE CAS CSCD 1993年第1期103-112,共10页
A method of linear momentum approximation is proposed that deals with weak nonlinear problems in an approximate manner. A motion of nonlinear nature is obtained in the system by assuming the motion to be in the form o... A method of linear momentum approximation is proposed that deals with weak nonlinear problems in an approximate manner. A motion of nonlinear nature is obtained in the system by assuming the motion to be in the form of linear momentum flow in the corresponding space introduced, followed by the transformation from the specified into a physical space. Significant results have been thereby derived in examining the effects of baroclinic Ekman momentum flow upon Eady-type baroclinic waves and frontogenesis. Also, this technique can be applied to investigate the dynamic characteristics of the weak nonlinear boundary layer including topography, stratification and non-Ekmantype friction for gaining further insight into the influence on the boundary layer inner parameters of terrain, baroclinicity and inhomogeneous process so that the classic theory is revised. 展开更多
关键词 Linear Momentum Approximation and frontogenesis Caused by Baroclinic Ekman Momentum Flow
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黄土高原两次对流暴雨特征及成因异同分析
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作者 屈丽玮 刘菊菊 +3 位作者 赵强 刘胜男 梁绵 潘留杰 《气象与环境科学》 2025年第2期33-44,共12页
运用高空和地面加密自动气象站观测资料及欧洲中心ERA-5(0.25°×0.25°)再分析资料,对2019年7月黄土高原陕西北部连续发生的两次暴雨过程的对流环境条件、触发机制进行诊断分析,探讨锋生作用和暴雨动力因子的异同点。结果... 运用高空和地面加密自动气象站观测资料及欧洲中心ERA-5(0.25°×0.25°)再分析资料,对2019年7月黄土高原陕西北部连续发生的两次暴雨过程的对流环境条件、触发机制进行诊断分析,探讨锋生作用和暴雨动力因子的异同点。结果表明:(1)两次过程副高位置稳定,“7·21”过程暴雨出现在700 hPa暖式切变线南部暖区中,低层偏南暖湿输送持续增强,整层水汽辐合较强,强降水区自南向北移动,为暖区对流降水。“7·28”过程700 hPa形成冷式切变线,整层水汽辐合较弱,局地湿度条件更好,高层干冷空气自北向南侵入低层,形成比湿锋区,局地雨强较大,强降水区由北向南移动,为锋面对流降水。(2)两次过程CAPE均为狭长型,“7·21”过程抬升凝结高度较低,暖云厚度大。“7·28”过程CAPE值较大,整层能量条件更好,对流不稳定度更强。(3)两次过程的触发机制不同,西路弱冷空气入侵形成的地面中尺度辐合线触发“7·21”暴雨产生,过程以层积混合云降水回波为主,深厚持久的偏南急流的长时间维持,产生列车效应,导致累积雨量大。“7·28”过程中层较强锋生作用造成的强烈上升运动触发对流降水,配合气旋式辐合,形成东北—西南向带状积云回波,单点降水强度更大。(4)两次过程的对流涡度矢量及云水含量大值区与强降水落区的演变相对应,“7·21”过程表现为由西南向东北移动的趋势,“7·28”过程表现为自西北向东南移动的趋势。可见,对流涡度矢量在暖区对流降水和锋面对流降水中可以表征不同的强降水变化特征,在预报中有一定的参考价值。 展开更多
关键词 对流暴雨 锋生函数 对流涡度矢量 触发机制
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逗点状MCS中的γ中尺度涡旋形成机制及结构特征
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作者 徐姝 王艳春 +3 位作者 王莹 庄园煌 易笑园 张文龙 《暴雨灾害》 2025年第5期642-652,共11页
利用自动站观测资料、多普勒天气雷达资料以及ERA5再分析等资料,对2022年7月5日夜间发生在渤海西岸的一次大暴雨过程进行观测和数值预报结果分析,初步探讨了逗点状中尺度对流系统(MCS)中的γ中尺度涡旋形成机制及其结构特征。结果表明:... 利用自动站观测资料、多普勒天气雷达资料以及ERA5再分析等资料,对2022年7月5日夜间发生在渤海西岸的一次大暴雨过程进行观测和数值预报结果分析,初步探讨了逗点状中尺度对流系统(MCS)中的γ中尺度涡旋形成机制及其结构特征。结果表明:暴雨过程发生在高空低槽东移和台风“暹芭”减弱后低压倒槽北抬的天气背景下,由逗点状中尺度对流系统头部的低质心涡旋回波有组织性地持续影响渤海西岸造成。γ中尺度涡旋最初发生在低压倒槽顶部,是由前期降水形成的西北气流和暖湿东南气流相遇后的锋生作用所致,其随后在925 hPa、850 hPa依次出现,降水主要出现在涡旋的右侧。涡度方程的收支诊断表明,涡旋主要由低层水平辐合辐散项提供初始扰动,后通过垂直涡度依次向上输送,最终在对流层下半部形成深厚的中尺度涡旋。涡旋在700—850 hPa附近存在暖心结构,925 hPa以下弱冷空气的渗透为对流雨带的发展提供了热力不稳定和动力强迫作用;涡旋呈现不对称结构特征,其东侧上升速度大于西侧,使得东侧降水明显强于西侧。涡旋的水汽输送也呈明显的不对称结构,水汽辐合主要集中在涡旋东侧即渤海西岸,这也是涡旋东侧降水偏强的原因。 展开更多
关键词 γ中尺度涡旋 锋生 不对称结构 暖心 涡度收支
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辽宁两次极端雨转暴雪过程对比分析
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作者 徐庆喆 徐爽 +4 位作者 金巍 田璐 高清源 谭政华 孙安妮 《干旱气象》 2025年第3期450-459,共10页
研究爆发性气旋背景下极端雨雪天气的形成机制,对冬季降水预测与雪灾防御具有重要意义。本文基于常规气象观测资料和ERA5再分析资料,从影响系统、水汽条件、动力机制及热力作用等方面,对比分析了2021年11月6—9日(简称“过程Ⅰ”)与2023... 研究爆发性气旋背景下极端雨雪天气的形成机制,对冬季降水预测与雪灾防御具有重要意义。本文基于常规气象观测资料和ERA5再分析资料,从影响系统、水汽条件、动力机制及热力作用等方面,对比分析了2021年11月6—9日(简称“过程Ⅰ”)与2023年11月5—7日(简称“过程Ⅱ”)辽宁地区两次极端雨转暴雪过程的成因与特征。结果表明,高空冷涡与地面爆发性气旋的共同作用是两次过程形成和发展的关键,高低空急流耦合为极端雨雪天气提供了强动力支撑,强降水主要分布在地面气旋北侧;条件性对称不稳定是两次极端雨雪天气的主要动力机制,低层锋区明显,水汽辐合区与锋区配合,有利于强降水形成。低层抬升运动、锋区与水汽辐合区的相位差异,是导致两次过程降水中心强度差异的主要原因。动力与水汽条件的共同作用以及温度条件共同决定降水相态,其中,低层冷锋强度及冷空气入侵时间影响降水相态的转变及雨雪分布。 展开更多
关键词 暴雪 爆发性气旋 雨转雪 锋生
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渤海湾飑线入海增强机制的个例研究
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作者 梅婵娟 王秀明 +2 位作者 李蕊 万夫敬 张莉萍 《气象》 北大核心 2025年第9期1061-1071,共11页
利用常规观测资料、雷达资料和ERA5再分析数据等,对2021年7月31日夜间影响渤海海区的一次强飑线过程的增强、维持物理过程进行了分析。结果表明:海岸地形、海表温度是影响入海飑线强度变化的关键因子。渤海中西部暖水区有着更好的热力... 利用常规观测资料、雷达资料和ERA5再分析数据等,对2021年7月31日夜间影响渤海海区的一次强飑线过程的增强、维持物理过程进行了分析。结果表明:海岸地形、海表温度是影响入海飑线强度变化的关键因子。渤海中西部暖水区有着更好的热力不稳定条件,且风速大值区与海表温度高值区相对应,渤海湾周边热力最不稳定,加上海岸喇叭口地形的“狭管效应”导致沿岸迎风一侧形成显著的风场辐合,有利于沿海对流的触发。初期,陆上多单体风暴形成的冷池出流与环境气流辐合使得风暴向东传播进入渤海湾,渤海湾北部复杂的海岸地形导致的非均匀向岸风有利于沿海分散雷暴单体新生,分散雷暴单体的多次并入使得陆上多单体风暴在沿海持续增强形成飑线。飑线入海后发展为“人字形”,伴随冷池合并,并有一中尺度涡旋使得飑线在渤海湾北部海岸线附近加强。在海上飑线加强过程中,暖水区及冷池相关的边界层锋生发挥着至关重要的作用,最终使得飑线在渤海暖水区发展加强,在冷水区减弱消散。 展开更多
关键词 飑线 海岸地形 海表温度 锋生
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