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21.
肖春喜  张华  刘泉声 《岩土力学》2004,25(5):835-838
详细地介绍了采用花管注浆的软托换技术,对紧邻边坡的建筑物地基进行加固处理,对开挖的边坡采取喷锚网结构支护这一技术在工程中的加固机理。实践表明,花管注浆联合喷锚网支护这种复合的加固方法,不仅能对紧邻边坡的建筑物的基础进行托换,还能对边坡进行有效地支护,保证了边坡的稳定性和建筑物的安全性,其设计方法具有一定的参考价值。  相似文献   
22.
南海台风与上层海洋相互作用的数值模拟研究   总被引:2,自引:2,他引:0       下载免费PDF全文
关皓  王汉杰  周林  杨松 《地球物理学报》2011,54(5):1141-1149
本文建立了一个综合考虑大气-海流-海浪相互作用的区域海-气耦合模式系统,利用该系统模拟研究了南海台风发生发展的大气、海洋动力学机理.结果表明:耦合模式较真实地反映了台风和上层海洋的相互作用过程,提高了对台风路径和强度的模拟准确率;在台风充分发展阶段,上层海洋的反馈作用使台风路径发生左偏,并抑制了台风强度的发展;三种海洋...  相似文献   
23.
In this study, the impact of atmosphere-wave coupling on typhoon intensity was investigated using numerical simulations of an idealized typhoon in a coupled atmosphere-wave-ocean modeling system. The coupling between atmosphere and sea surface waves considered the effects of wave state and sea sprays on air-sea momentum flux, the atmospheric low-level dissipative heating, and the wave-state-affected sea- spray heat flux. Several experiments were conducted to examine the impacts of wave state, sea sprays, and dissipative heating on an idealized typhoon system. Results show that considering the wave state and sea-spray-affected sea-surface roughness reduces typhoon intensity, while including dissipative heating intensifies the typhoon system. Taking into account sea spray heat flux also strengthens the typhoon system with increasing maximum wind speed and significant wave height. The overall impact of atmosphere-wave coupling makes a positive contribution to the intensification of the idealized typhoon system. The minimum central pressure simulated by the coupled atmosphere-wave experiment was 16.4 hPa deeper than that of the control run, and the maximum wind speed and significant wave height increased by 31% and 4%, respectively. Meanwhile, within the area beneath the typhoon center, the average total upward air-sea heat flux increased by 22%, and the averaged latent heat flux increased more significantly by 31% compared to the uncoupled run.  相似文献   
24.
In this paper,the effects of sea spray on tropical cyclone(TC)structure and intensity variation are evaluated through numerical simulations using an advanced sea-spray parameterization from the National Oceanic and Atmospheric Administration/Earth System Research Laboratory(NOAA/ESRL),which is incorporated in the idealized Advanced Research version of the Weather Research and Forecast (WRF-ARW)model.The effect of sea spray on TC boundary-layer structure is also analyzed.The results show that there is a significant increase in TC intensity when its boundary-layer wind includes the radial and tangential winds,their structure change,and the total surface wind speed change.Diagnosis of the vorticity budget shows that an increase of convergence in TC boundary layer enhances TC vorticity due to the dynamic effect of sea spay.The main kinematic effect of the friction velocity reduction by sea spray produces an increment of large-scale convergence in the TC boundary layer,while the radial and tangential winds significantly increase with an increment of the horizontal gradient maximum of the radial wind, resulting in a final increase in the simulated TC intensity.The surface enthalpy flux enlarges TC intensity and reduces storm structure change to some degree,which results in a secondary thermodynamic impact on TC intensification.Implications of the new interpretation of sea-spray effects on TC intensification are also discussed.  相似文献   
25.
It has long been recognized that the evolution ot marine storms may De strongly alIected Dy the nuxtransfer processes over the ocean. High winds in a storm can generate large amounts of spray, which canmodify the transfer of momentum, heat, and moisture across the air-sea interface. However, the role of seaspray and air-sea processes in western Pacific typhoons has remained elusive. In this study, the impact ofsea spray on air-sea fluxes and the evolution of a typhoon over the western Pacific is investigated using acoupled atmosphere-sea-spray modeling system. Through the case study of the recent Typhoon Fengshenfrom 2002, we found that: (1) Sea spray can cause a significant latent heat flux increase of up to 40% ofthe interfacial fluxes in the typhoon; (2) Taking into account the effects of sea spray, the intensity of themodeled typhoon can be increased by 30% in the 10-m wind speed, which may greatly improve estimatesof storm maximum intensity and, to some extent, improve the simulations of overall storm structure in theatmospheric model; (3) The effects of sea spray are mainly focused over the high wind regions around thestorm center and are mainly felt in the lower part of the troposphere.  相似文献   
26.
To study the potential effect of sea spray on the evolution of typhoons,two kinds of sea spray flux parameterizationschemes developed by Andreas (2005) and Andreas and Wang (2006) and Fairall et al.(1994) respectively are incorporated into theregional atmospheric Mesoscale Model version 3.6 (MM5V3) of Pennsylvania State University/National Center for AtmosphericResearch (PSU/NCAR) and the coupled atmosphere-sea spray modeling system is applied to simulate a Western Pacific super ty-phoon Ewiniar in 2006.The simulation results demonstrate that sea spray can lead to a significant increase in heat fluxes at theair-sea interface and the simulated typhoon's intensity.Compared with the results without sea spray,the minimum sea level pressurereduces about 8hPa after taking account of sea spray by Fairall et al.'s parameterization (1994) and about 5hPa by Andreas' (2005)and Andreas and Wang's (2006) parameterization at the end of the model integration,while the maximum 10m wind speed increasesabout 17% and 15% on average,respectively,through the entire simulation time period.Taking sea spray into account also causessignificant changes in Tropical Cyclone (TC) structure due to an enhancement of water vapor and heat transferred from the sea sur-face to the air; therefore,the center structure of the typhoon becomes more clearly defined and the wind speed around the typhooneye is stronger in numerical experiments.The simulations show that different sea spray flux parameterizations make different modifications to the TC structure.  相似文献   
27.
旋喷注浆及静压注浆在公路路基加固中的运用   总被引:1,自引:0,他引:1  
胡强 《安徽地质》2006,16(4):290-291,294
安庆铜矿3#矿体公路部分路基处于地表塌陷区,由于地下水的潜蚀作用,导致路基出现大幅度的沉降和开裂。为此,对该路基采用了旋喷注浆和静压注浆加固,使不均匀和开裂得到了有效的控制。  相似文献   
28.
海浪和海洋飞沫对“珊珊”台风影响的数值研究   总被引:1,自引:0,他引:1  
刘磊  费建芳  郑静  程小平 《气象学报》2011,69(4):693-705
台风是剧烈的天气系统,在开放的海上强风激起大浪,改变了海表粗糙度,同时,海浪顶端的白泡沫破碎,在海-气界面处会出现大量的海洋飞沫。基于共享内存的进程间通信技术应用到区域大气和海浪模式的耦合中,大气模式引入了Fairall和Andreas两种海洋飞沫参数化方案,对2006年珊珊台风进行了模拟对比试验,结果表明:耦合模式通过海-气相互作用,对台风的强度产生影响,由于耦合模式在海表粗糙度的计算上考虑了海表状况,使得耦合模式模拟的台风强度更接近实况,而对台风的移动路径影响不大;耦合模式中海-气相互作用主要通过动力因素来对台风产生影响,海表状况影响了海表粗糙度,从而使台风的动量输送发生变化,具体的台风强度增强还是减弱主要取决于海表状况与实况的符合程度;海洋飞沫参数化主要通过热力场的改变来影响动力场,Fairall方案中潜热通量和感热通量得到很大程度的加强,使得台风的热力结构得以改变,台风强度明显加强,从而影响了动力场结构;Andreas方案由于其界面通量算法在高相对湿度条件下计算界面通量时得到的量值较小,虽然高风速条件下感热通量加大,但总的潜热通量、感热通量较Fairall方案为弱,因此,模拟的台风强度不强;海洋飞沫参...  相似文献   
29.
本文以2006年9月日本以南海域的台风YAGI为例,应用黑潮延伸体附近的KEO浮标观测资料,并结合卫星遥感等融合资料,分析海洋飞沫在台风不同发展阶段对海气界面间热量通量和动量通量的影响。首先,定量地分析台风期间海洋飞沫对海气热通量的影响。结果表明,在台风YAGI过境期间,海洋飞沫能够显著地加剧海气界面间的热量交换,尤其是潜热交换。海洋飞沫增加的热通量随着风速的增强而增大,随着波龄的增大而减小。随后,通过动量分析表明,在台风YAGI过境期间,海洋飞沫显著地增强了由大气向海洋的动量转移。当风速达到台风量级后,考虑海洋飞沫所增加的动量通量与界面动量通量大小相当,同时,在此风速条件下,海洋飞沫在海气界面形成极限饱和悬浮层,抑制风到海表面的动量转移,导致海气界面间总的动量通量的增长率随之减小。  相似文献   
30.
The dispersion of heavy particles and pollutants is often simulated with Lagrangian stochastic (LS) models. Although these models have been employed successfully over land, the free surface at the air-sea interface complicates the implementation of traditional LS models. We present an adaptation of traditional LS models to the atmospheric marine boundary layer (MBL), where the bottom boundary is represented by a realistic wavy surface that moves and deforms. In addition, the correlation function for the turbulent flow following a particle is extended to the anisotropic, unsteady case. Our new model reproduces behaviour for Lagrangian turbulence in a stratified air flow that departs only slightly from the expected behaviour in isotropic turbulence. When solving for the trajectory of a heavy particle in the air flow, the modelled turbulent forcing on the particle also behaves remarkably well. For example, the spectrum of the turbulence at the particle location follows that of a massless particle for time scales approximately larger than the Stokes’ particle response time. We anticipate that this model will prove especially useful in the context of sea-spray dispersion and its associated momentum, sensible and latent heat, and gas fluxes between spray droplets and the atmosphere.  相似文献   
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