10──20天准双周振荡的经向传播及地理特征   总被引：1，自引：0，他引：1  

武炳义  章淹．家英杰 《大气科学》1994,(5)

本文采用ＥＣＭＷＦ１９８３年７月１日至９月１２日逐日２００ｈＰａ纬向风场资料，用复经验正交方法讨论了１０－２０天低频振荡的经向传播及地理特征。结果表明：（１）１０－－２天振荡有三个显著区域：贝加尔湖附近地区；赤道９０°Ｅ附近以及新加坡、马来西亚地区；８０－１００°Ｅ，２２－３２°Ｎ之间。（２）源于较高纬度地区的振荡与源于赤道附近地区的振荡在１０５°Ｅ，１７—２３°Ｎ附近同位相相遇，在９０°Ｅ，２０°Ｎ附近反位相相叠加，振荡相互削弱，在２５°Ｎ附近同位相相遇。（３）从振荡位相来看，中南半岛东南部、马来西亚北部、菲律宾以西区域的振荡向北传播到中国东南沿海，向西传播到孟加拉湾印度半岛；２０°Ｎ以南低纬度地区的振荡很少能传播到８０°Ｅ以东３０°Ｎ附近地区；位于９０－９５°Ｅ，２５－２７°Ｎ之间的振荡以及贝加尔湖附近地区的振荡可以向南北两个方向传播。  相似文献   

类透镜介质中的传导模及与激光束的耦合     

翁兴涛 《武汉大学学报(信息科学版)》1994,(4)

从求解柱坐标内亥姆霍兹方程出发，导出了类透镜介质传导模的特征参量、场分布状态及传播常数，求出了入射激光束和导模之间的耦合系数，并讨论了它们的物理意义．  相似文献   

经圈环流对定常波传播的影响   总被引：1，自引：0，他引：1  

宋燕  缪锦海 《气象学报》1994,52(4):424-432

在一般斜压大气中，基本气流中包含经圈环流时，定常波传播不仅能穿过东风带，而且明显增强。在基流含有经圈环流的情况下，北半球中纬度地形强迫可引起低纬大气的显著响应，这表明经圈环流在中低纬定常响应的相互联系中起着重要作用；北半球中纬度热力强迫可产生类似北半球夏季季风环流的波列分布，这说明经圈环流在夏季季风环流的形成中起着一定的作用；在赤道东太平洋加热强迫情况下，在冬半球可引起ＰＮＡ型的定常波传播波列，而在夏半球却没有明显的ＰＮＡ特征。这表明经圈环流对冬、夏半球的定常波传播路径有着显著的影响。  相似文献   

A numerical simulation of gas flow during coal/gas outbursts   总被引：2，自引：0，他引：2  

F. Otuonye  J. Sheng 《Geotechnical and Geological Engineering》1994,12(1):15-34

Summary A model of the gas flow in airways during an instantaneous outburst of coal and gas is formulated and solved numerically using MacCormack's explicit finite-difference scheme. This model is based on the assumption that geological structures, in-situ stresses and high-gas-pressure gradients play important roles in initiating an outburst, with the gas content and gas-pressure gradients being the most dominant factors. The fluid-dynamic processes that occur after an outburst are computed by the numerical integration of the complete time-dependent Navier-Stokes equations. The mixture velocity, the density and the gas-concentration profiles in both time and space domains (immediately after an outburst) are presented. The global results are useful in gaining an improved understanding of gas-flow patterns during coal/gas outbursts and in determining the range of the disturbance so that effective methods of control can be developed.Nomenclature a speed of sound - C gas concentration (mass) - C _v specific heat at constant volume - C _p specific heat at constant pressure - CFL Courant-Friedrichs-Lewy number - E total energy of the mixture - F the vector defined in Equation 27 - G the vector defined in Equation 28 - h entropy - h _i entropy at inlet - J _xi diffusion flux in the i-direction - k thermal conductivity of a gas - M Mach number - P pressure of a mixture (the partial pressure of gas) - P gas pressure - P _a atmospheric pressure  相似文献   

1989年7月川东大暴雨中尺度对流系统分析   总被引：2，自引：2，他引：2       下载免费PDF全文

项续康 《气象》1995,21(3):30-34

使用气象卫星资料，分析了１９８９年７月发生在四川东部的４个中尺度对流系统的特征，第一个系统是由３个对流云团合并而成，生成后快速向前移动，第二个为向后传播。第三个系统生成后，系统的西南部不断生成新的对流单体，使之维持准静止状态，最后一个系统的初期呈胞状结构，后与冷锋结合，成为冷锋云系的一部分，这４个系统都是西南低涡暖切变形势下的产物，随着形势演变，其大尺度环境略有差异。  相似文献   

横向非均匀介质中弹性地震波传播的数值模拟     

张剑峰  李幼铭 《地震工程与工程振动》1995,15(3):21-31

应用混合变量弹性动力学方程和线性常微分方程组的矩阵指数解法，将层状介质中广泛应用的弹性波传播矩阵解法推广至横向非均匀介质，给出了一种可计算复杂地质体中弹性波传播的广义传播矩阵数值解法。该方法可模拟任意震源及所产生的各种体波、面波，数值结果表明具有很高的计算精度。  相似文献   

大气传播延迟改正在GAMIT软件中的应用   总被引：4，自引：1，他引：3       下载免费PDF全文

张清志 《沉积与特提斯地质》2001,21(2):23-30

卫星信号从GPS卫星发射到地面的过程中经过了以充满大气为介质的空间,电磁波在这种变化的介质中传播,其传播的方向、速度、强度都可能随时改变,本文简略地介绍了大气传播延迟的产生及其对GPS测量的影响,并就GAMIT软件对大气传播延迟的控制方法和所采用的改正模型做一简单介绍,并对减弱和消除大气传播延迟的方法和手段进行了讨论。  相似文献   

Run-up from impact tsunami     

D. G. Korycansky  Patrick J. Lynett 《Geophysical Journal International》2007,170(3):1076-1088

We report on calculations of the on-shore run-up of waves that might be generated by the impact of subkilometre asteroids into the deep ocean. The calculations were done with the COULWAVE code, which models the propagation and shore-interaction of non-linear moderate- to long-wavelength waves  ( kh < π)  using the extended Boussinesq approximation. We carried out run-up calculations for several different situations: (1) laboratory-scale monochromatic wave trains onto simple slopes; (2) 10–100 m monochromatic wave trains onto simple slopes; (3) 10–100 m monochromatic wave trains onto a compound slope representing a typical bathymetric profile of the Pacific coast of North America; (4) time-variable scaled trains generated by the collapse of an impact cavity in deep water onto simple slopes and (5) full-amplitude trains onto the Pacific coast profile. For the last case, we also investigated the effects of bottom friction on the run-up. For all cases, we compare our results with the so-called 'Irribaren scaling': The relative run-up   R / H ₀=ξ= s ( H ₀/ L ₀)^−1/2  , where the run-up is   R , H ₀  is the deep-water waveheight, L ₀ is the deep-water wavelength, s is the slope and ξ is a dimensionless quantity known as the Irribaren number. Our results suggest that Irribaren scaling breaks down for shallow slopes   s ≤ 0.01  when  ξ < 0.1 − 0.2  , below which   R / H ₀  is approximately constant. This regime corresponds to steep waves and very shallow slopes, which are the most relevant for impact tsunami, but also the most difficult to access experimentally.  相似文献   

Lamb's problem with the lattice model Mka3D     

C. Mariotti 《Geophysical Journal International》2007,171(2):857-864

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High-resolution structures of the Landers fault zone inferred from aftershock waveform data   总被引：2，自引：0，他引：2  

Hongyi Li  Lupei Zhu  Hongfeng Yang 《Geophysical Journal International》2007,171(3):1295-1307

High-frequency body waves recorded by a temporary seismic array across the surface rupture trace of the 1992 Landers, California, earthquake were used to determine fault-zone structures down to the seismogenic depth. We first developed a technique to use generalized ray theory to compute synthetic seismograms for arbitrarily oriented tabular low-velocity fault-zone models. We then generated synthetic waveform record sections of a linear array across a vertical fault zone. They show that both arrival times and waveforms of P and S waves vary systematically across the fault due to transmissions and reflections from boundaries of the low-velocity fault zone. The waveform characteristics and arrival-time patterns in the record sections allow us to locate the boundaries of the fault zone and to determine its P - and S -wave velocities independently as well as its depth extent. Therefore, the trade-off between the fault-zone width and velocities can be avoided. Applying the method to the Landers waveform data reveals a low-velocity zone with a width of 270–360 m and a 35–60 per cent reduction in P and S velocities relative to the host rock. The analysis suggests that the low-velocity zone extends to a depth of ∼7 km. The western boundary of the low-velocity zone coincides with the observed main surface rupture trace.  相似文献