排序方式： 共有53条查询结果，搜索用时 484 毫秒
1.
2.
本文对0421(海马)和0311(环高)台风登陆后不同的演变过程进行了对比分析。分析表明,虽然两次台风登陆的时间和路径都很相似,但是由于环境场的形势的不同,特别是北方冷空气情况的不同,一个变性发展成为温带气旋,给江苏地区带来了大面积的降水,另一个直接减弱消失,仅在登陆点附近产生了一些降水。通过讨论锋生函数各项的性质和计算其主要项的分布特征,对变性过程进行了研究,发现台风变性初期其锋生函数中变形项起主要作用。锋生结果造成强烈的辐合上升运动,引起台风暴雨的增幅。 相似文献
3.
地面锋附近重力流的产生及其锋生作用 总被引：3，自引：0，他引：3
本文用旋转大气的两维非静力模型,用Simpson和Linden[1]的级数展开方法和数值积分方法讨论了地面锋附近由于非地转平衡所产生的重力流及锋生作用。 相似文献
4.
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 de-creasing 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 tempera-ture gradient can make the final energy conversion ratio higher, and vice versa; (3) suitable vapor distribu-tion is favorable for the frontogenesis. It will bring forward the time of the frontogenesis, strengthen the in-tensity of the cold front, and influence the final energy conversion ratio; (4) the orographic forcing has an ev-idently strengthening effect on the frontogenesis. The strengthening effect on the frontogenesis and the influ-ence on the final energy conversion ratio depend on the relative location of the mountain to the cold front. 相似文献
5.
High frequency wind and temperature measurements, obtained in March 1995 from a 10-m tower array situated in south-east Kansas, are used to analyze the structure of a shallow density current. This current is approximately 7 m deep and exhibits a current head that is estimated to be about twice the current depth. The event lasted approximately 900 s and its origin appears to be a shallow slope 2–:5 km to the west of the site, where cold air drainage occurs. The onset of the event is marked by a 5 °C temperature decrease at the 3-m level, increased variance of temperature and of wind velocity, and increased dissipation of kinetic energy, measured by a hot-wire anemometer at the 3-m level. The primary contributors to temperature changes following the frontal passage are both horizontal and vertical advections; contributions from flux divergences of temperature and of radiation, and from dew formation, do not appear to be significant. Postulated frontogenesis, prior to the arrival of the apparent equilibrated front of approximately 176-m width at the site, is examined by means of a theoretical model. The time required to equilibrate the front, by means of kinetic energy dissipation within the frontal zone, is determined to be less than 300 s, or less than the estimated travel time from the orographic slope to the observational site. The absence of upstream data is determined, however, to be a limitation of the analysis performed. 相似文献
6.
A Diagnostic Study of Explosive Development of Extratropical Cyclone over East Asia and West Pacific Ocean 总被引：9，自引：0，他引：9
ＡＤｉａｇｎｏｓｔｉｃＳｔｕｄｙｏｆＥｘｐｌｏｓｉｖｅＤｅｖｅｌｏｐｍｅｎｔｏｆＥｘｔｒａｔｒｏｐｉｃａｌＣｙｃｌｏｎｅｏｖｅｒＥａｓｔＡｓｉａａｎｄＷｅｓｔＰａｃｉｆｉｃＯｃｅａｎ￥ＪｉａＹｉｑｉｎ（贾逸勤）ａｎｄＺｈａｏＳｉｘｉｏｎｇ（赵思雄）（... 相似文献
7.
Simple model flows demonstrating the combined effect of thermobaricity with either salinity variations or nonlinear temperature-dependence in the equation of state of water are investigated. An inviscid flow exhibits a three-layer behaviour, resulting in the formation of a mid-depth temperature maximum, such as is observed in some high-latitude oceans and deep lakes. This may be subsequently overtaken by nonlinear frontogenesis, which in the viscous case is shown to generate a thermal bar. Thermobaricity shifts the thermal bar towards the cold water, and initially produces a slope in the downwelling plume, but this transient feature disappears as the dominant frontogenesis tilts the plume back to the vertical. 相似文献
8.
作者的目的是分析地形对由于热力差异所引起的局地锋生现象和地转适应过程的影响．为此，分别用零位涡流和均匀位涡流来近似代替实际大气，并借助位涡、绝对动量、位温的守恒关系，就地形对适应锋生和适应过程中能量转换等问题进行了简单讨论。初始位温扰动的水平分布及其相对于地形的位置对适应锋生有重要影响。当初始热力扰动主要位于地形迎风坡山脚时，地形不利于锋面形成，这时要形成锋面不连续，初始位温梯度的水平变化必须非常显著；当初始热力扰动主要位于山顶附近时，地形促进流体运动的辐合，有利于锋面不连续的形成，这时即使初始位温梯度的水平变化不是很大，也可能会形成锋面；当初始热力扰动主要位于背风坡时，地形是否有利于锋面不连续的形成取决于流体的层结情况，如果流体的基本层结很弱，地形促进锋面不连续的形成，反之，地形不利于锋面不连续的形成，这种差异主要是由于在这两种情况下，地形引起的下沉增温效应的强弱是不同的。另外，地形对地转适应过程中动能和位能之间的能量转换率也有影响，与没有地形的情况相比，当初始热力差异显著区位于迎风坡时，能量转换率减小，当不平衡场位于背风坡时，能量转换率增加，原因是在迎风坡流体要克服重力作功，在背风坡重力对流体作正功。 相似文献
9.
一次冬季锋面暴风雪天气过程的斜压边界层特征的观测分析 总被引：4，自引：0，他引：4
对STORM-FESTIOP17一次冬季锋面暴风雪天气过程的斜压边界层结构演变及特征进行了分析。发现：暖湿空气沿锋面抬升凝结成云，产生降水过程中释放的大量潜热显著增加锋两侧的水平温度差异，产生锋生。与锋生相伴，在锋前产生低空急流和高空急流。当锋生至最强时，锋两侧温差可达20K，锋前低空急流开始减弱，锋后低空急流增强，锋后冷平流开始主导锋两侧的环流系统。该冷平流削弱锋两侧的温度水平梯度，产生锋消作用。对这次锋面斜压对流边界层的湍流特征分析表明：在边界层之上切应力wv明显增大；湍能收支分析表明在边界层之上的风切变产生项很强，即大尺度天气系统有利于斜压对流边界层的发展，边界层内各量充分混合。这次冬季锋面暴风雪天气过程，冷锋前的低空南风急流从墨西哥湾携带来的充足水汽及锋区边界层大气的强斜压性是其产生的关键因子：冷锋过后，大尺度高空急流的作用更有利于对流边界层的充分发展。 相似文献
10.
用10层准拉格朗日有限区域模式对高原东侧锋生过程的数值模拟 总被引：2，自引：1，他引：2
本文对一次引起夏季华北暴雨的锋生过程进行了研究。在诊断分析的基础上,我们采用十层准拉格朗日有限区域模式对此个例进行了48小时的模拟,并对模拟输出结果进行解释与再次诊断。表明:(1)夏季高原东侧有时两支气流交绥很清楚,温度对比明显,与梅雨锋的情况很不相同,这在夏末尤其如此。这种温度对比区虽比冬季弱,但是,与夏季天气系统的发展及降水是有关系的。(2)模拟结果与实际观测资料是很相似的,再现了两支气流形成切变线的三维结构、移动与演变,并模拟出了在对流层中存在着深厚的24小时变温区;模拟发现,一条东北-西南向的锋生 相似文献