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1.
台风的螺旋结构 总被引：14，自引：3，他引：14
本文从描写台风运动的动力方程组出发,讨论了台风的螺旋结构,给出了这种螺旋结构的图样,指出:(1)台风螺旋结构的形成是台风中重力惯性内波,特别是重力内波的作用所致,(2)台风螺旋结构的形式与波位相速紧密相关,北半球的曳式螺旋结构要求螺旋图样环绕台风眼逆时针且由中心向外运动,其向外运动的速度近于重力内波的传播速度,(3)台风的曳式螺旋倾角一般小于45°,而在台风边缘,倾角约为10°,螺旋臂间距在二旋臂结构中平均为220公里,而在四旋臂结构中平均为110公里,(4)台风螺旋波也有频散作用,在曳式螺旋中c_(gr)与c_r皆为正,且c_(gr)相似文献
2.
本文归纳总结了在绝热、无耗散对称二维大气中定常广义地转流稳定性分析中的扰动方程组的基本特征，并将其概括为具有这类问题共同基本特征的统一形式的扰动方程组的定解问题。在此基础上，统一地证明了：１）由统一的扰动方程组所确定的定解问题的解是存在唯一的；２）基态的性质是由Λｍｉｎ（Ｇ）的性质决定的：ａ．当Λｍｉｎ（Ｇ）＞０时，基态是稳定的；ｂ．当Λｍｉｎ（Ｇ）＜０时，基态是不稳定的。３）基态的全局稳定性质可以通过局部稳定性分析来确定；４）合理的、充分简化的局部稳定性分析结论在局部分析中是严格有效的 相似文献
3.
THE EFFECTS OF VERTICAL VARIATION OF BASIC FLOW AND HORIZONTAL GRADIENT OF TEMPERATURE ON LINEAR AND NONLINEAR GRAVITY WAVES 
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下载免费PDF全文 By using two-dimensional dynamical equations in x-z plane with Boussinesq approximation,the effects of the second-order vertical shear of the basic flow uzz and the horizontal gradient of temperature (M) on the gravity wave and the isolated gravity wave are discussed.The magnitudes of uzz and M corresponding to the linear and nonlinear stabilities of the gravity waves are worked out,respectively.The results show that amplitude and width of the isolate dgravity wave are closely related to uzz and M.It is indicated that the isolated gravity wave with a width of about 10 km can be motivated by the disturbance of sub-synoptic scale in the certain ranges of flow field shear and temperature gradient,while the motivated waves may be associated with the cold surge ahead of a cold front and the other mesoscale synoptic systems. 相似文献
4.
Adrian DeHeer-Amissah Ulf Högström Ann-Sofi Smedman-Högström 《Boundary-Layer Meteorology》1981,20(1):35-49
A set of semi-continuous measurements of temperature, wind and moisture gradients as well as of net radiation and ground heat flux covering a period of about one and a half years has been analysed to give a corresponding set of complete surface energy balance data on an hourly basis. An analysis of the evaporation data so obtained is given.It is shown that surface resistance r
S exhibits a diurnal trend: values are smallest (ca. 150 s m-1) a few hours before noon and increase to as much as 800 s m-1 towards dusk. The minimum values tend to be higher during dry periods when the soil moisture is low. There is also some indication that r
S decreases rapidly soon after rainfall.An exponential relation is found between the fraction of available energy used as evaporative flux, , and r
S for values of r
I/rS <0.70, where r
I is the climatological resistance. On the other hand, the ratio of r
I to r
S is linearly correlated with , implying that an equilibrium state is established between the grass surface and the atmosphere, at least from mid-morning to mid-afternoon when the leaves are dry. Near-noon values calculated by Stewart and Thom for Thetford Forest also follow a linear trend.The above two regression results (In (r
S) versus r
I/rS versus ) are combined to obtain an empirical relation of the form r
I=m exp (a-b) which is used to estimate evaporative flux. The estimates are found to be within 20% of calculated values.Guest Scientist from Department of Physics, University of Cape Coast, Cape Coast, Ghana. 相似文献
5.
不同生育期水分胁迫对玉米光合特性的影响 总被引：6，自引：0，他引：6
利用遮雨棚以夏玉米为对象进行水分胁迫大田试验,通过分析玉米叶片光合测量数据,研究不同生育期水分胁迫对玉米光合特性的影响,为定量分析不同水分胁迫程度对玉米生育的可能机理提供数据和初步的理论支持.结果表明:土壤水分下降会使玉米叶片的光合速率(Pn)、气孔导度(Gs)、蒸腾速率(Tr)降低,而胞间CO2浓度(Ci)和水分利用效率(WUE)会增加;Pn随着光照强度的增加而增加,且随着水分胁迫强度增强,Pn增加速率降低;干旱胁迫会改变Pn、Tr日变化规律,并且对拔节期光合作用的抑制小于成熟期;WUE与Pn存在极显著的正相关关系,与Tr、Ci及Gs存在显著的负相关关系. 相似文献
6.
Comparisons of xylem sap flow and water vapour flux at the stand level and derivation of canopy conductance for Scots pine 总被引：7，自引：0，他引：7
A. Granier P. Biron B. Köstner L. W. Gay G. Najjar 《Theoretical and Applied Climatology》1996,53(1-3):115-122
Summary Simultaneous measurements of xylem sap flow and water vapour flux over a Scots pine (Pinus sylvestris) forest (Hartheim, Germany), were carried out during the Hartheim Experiment (HartX), an intensive observation campaign of the international programme REKLIP. Sap flow was measured every 30 min using both radial constant heating (Granier, 1985) and two types of Cermak sap flowmeters installed on 24 trees selected to cover a wide range of the diameter classes of the stand (min 8 cm; max 17.5 cm). Available energy was high during the observation period (5.5 to 6.9 mm.day–1), and daily cumulated sap flow on a ground area basis varied between 2.0 and 2.7 mm day–1 depending on climate conditions. Maximum hourly values of sap flow reached 0.33 mm h–1, i.e., 230 W m–2.Comparisons of sap flow with water vapour flux as measured with two OPEC (One Propeller Eddy Correlation, University of Arizona) systems showed a time lag between the two methods, sap flow lagging about 90 min behind vapour flux. After taking into account this time lag in the sap flow data set, a good agreement was found between both methods: sap flow = 0.745* vapour flux,r
2 = 0.86. The difference between the two estimates was due to understory transpiration.Canopy conductance (g
c
) was calculated from sap flow measurements using the reverse form of Penman-Monteith equation and climatic data measured 4 m above the canopy. Variations ofg
c
were well correlated (r
2 = 0.85) with global radiation (R) and vapour pressure deficit (vpd). The quantitative expression forg
c
=f (R, vpd) was very similar to that previously found with maritime pine (Pinus pinaster) in the forest of Les Landes, South Western France.With 6 Figures 相似文献
7.
In order to investigate flows over topography in an atmospheric context, we have studied experimentally the wake structure of axi-symmetric Gaussian obstacles towed through a linearly stratified fluid. Three dimensionless parameters govern the flow dynamics: F, the Froude number based on the topography height h; Re, the Reynolds number and the aspect ratio r = h/L, where L is the topography horizontal scale. Two-dimensional (2-D), saturated lee wave (SLW) and three-dimensional (3-D) regimes, as defined in Chomaz et al. (1993), are found to be functions of F and r only (Fig. 1) as soon as Re is larger than Rec ≈ 2000. For F < 0.7 the flow goes around the obstacle and the motion in the wake is quasi-two-dimensional. This 2-D layer is topped by a region affected by lee wave motions with amplitude increasing with r and F. For 0.7 < F < 1/r, the flow is entirely dominated by a lee wave of saturated amplitude which suppresses the separation of the boundary layer from the obstacle. Above the critical value 1/r, the lee wave amplitude decreases with F and a recirculating zone appears behind the obstacle. Simultaneously, coherent large-scale vortices start to be shed periodically from the wake at a Strouhal number which decreases as 1/F until it reaches its neutral asymptotic value. 相似文献
8.
Using the lAP two-level general circulation model,the ice age July climate was simulated through the surface conditions of 18 000 years before present assembled by the CLIMAP Project.Comparing with the present July simulation results,the ice age atmosphere is found to have a substantially lower temperature,precipitation,and cloudiness,higher sea-level pressure,especially in the high latitude land region of the Northern Hemisphere and Antarctica.When the CO2 content is set as the modern value the climatic response is very small,which shows that the problems of CO2 sensitivity should be studied by means of coupled models.It is also pointed out that there are some common characteristics between CO2-induced climatic changes and the ice age surface condition-induced climatic changes,which may give us some insight into how climate responds to external forcings. 相似文献
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本文应用Ｈｏｗａｒｄ（１９６１）所用的精巧积分方法研究了三维非静力平衡层结大气随高度变化基流上重力内波的不稳定性质。给出了不稳定产生的必要条件和相速度在相速复平面上的分布规律；发展了Ｍｉｌｅｓ定理和Ｈｏｗａｒｄ半圆定理；得到了有限深度气层的半椭圆定理。并指出在随高度变化的基流中，重力内波的不稳定范围与基流的垂向结构及波传播方向有关；半椭圆的位置和长轴分别重合于Ｈｏｗａｒｄ半圆的位置和直径，而短轴则依赖于与Ｒｉｃｈａｒｄｓｏｎ数相关的参数Ｊ０，Ｒ０和波数｜ｋ｜及流场厚度参数ｋ０ 相似文献
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13.
本文第一部分运用相似理論和因次分析对层結大气近地面层中湍流交換的問題作了分析,获得了与作者过去根据湍流能量平衡方程所得到的結果一致.第二部分根据新近国外发表的直接測量资料确定了普遍函数中的經驗系数D的大小;还确立了强迫对流向自由对流状态的过渡,与Priestley所指出的不同,它具有极平緩的性貭,計算結果与观測事实符合.在稳定情况下則沒有类似过渡发生.第三部分根据因次分析构成了特征尺度L_(R_i),并建立了以L_(R_i)为特征尺度的湍流交換的模式.討論結果表明,采用这一模式比前一模式合理一些,而且实用上更为方便。 相似文献
14.
A modified version of the Biome4 vegetation model for simulation of the mean δ13C of plant communities is presented, and used to reconstruct palaeoprecipitation. We treat all fractionations by C3 and C4 plants in all coexistent Plant Functional Types, weighted by their respective net primary production. We constrain the range of variation in the intracellular versus atmospheric CO2 concentration by fixing a lower limit. Finally, we replace some constant parameters by functions of external forcing to account for their responses to environmental variation. The new version of Biome4 was applied as an inverse model and tested on three modern data sets. The fit between observations and simulations is very close to the 1:1 relationship, with respective slopes of 0.90±0.02 (r 2=0.98, n=29) for δ13C and 0.97±0.06 (r 2=0.90, n=29) for precipitation. Inverse modelling was applied using the Metropolis-Hastings algorithm to the Nußloch loess sequence. Over the last glaciation, simulated palaeoprecipitation varies between 240 mm year?1 and 400 mm year?1. This study clearly demonstrates atmospheric teleconnections with the Greenland ice-sheet extension, by matching Dansgaard-Oeschger events with precipitation increase of ca. 100–200 mm year?1. 相似文献
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16.
Zhao Ming 《Boundary-Layer Meteorology》1983,26(3):209-226
The equations of motions are solved for concentric circular flow in the planetary boundary layer (PBL) under the assumption of K = l 2|?v/?z| and gradient wind independent of radius r. The theoretical distribution of wind is obtained for r ≥ 300 km. Other parameters of the PBL are also calculated. Finally, equilibrium of the forces in the PBL is analyzed. 相似文献
17.
Sensible Heat Flux-Radiometric Surface Temperature Relationship Over Sparse Vegetation: Parameterizing B-1 总被引：1，自引：0，他引：1
In the bulk formulation of vegetation-atmosphere transfer, theparameter B-1 is needed for evaluating the sensible heatflux from radiometric surface temperature. An excess resistance,expressed as a function of B-1 (rrB-1/u*, whereu* is the friction velocity), shouldbe added to the aerodynamic resistance calculated between thelevel of apparent sink of momentum and the reference height.Over sparse vegetation, B-1 (and consequently the excessresistance) can be very large and variable. A one-dimensionaltwo-layer model of the canopy-atmosphere interaction is used toinvestigate the behaviour of this fitting parameter and to derive anoperational parameterization in terms of structural and viewingcharacteristics. Besides canopy structural characteristics andradiometer viewing angle, input variables include weather data,stomatal and substrate resistances. B-1 varies with almostall the input variables; however, the leaf area index (LAI) andthe view angle of the radiometer appear as the most significantfactors of variation. Using a set of weather data and componentresistances randomly generated between fixed limits, `average'curves representing B-1 as a function of LAI for differentview angles are inferred from the model and polynomial expressionsare fitted to the simulated curves. This set of parameterizations isobtained from ranges of input data wide enough to be representativeof a large variety of experimental conditions. It is successfully testedagainst other parameterizations, using both simulated data andmeasurements made over contrasted surfaces in Niger, France andCalifornia. As the formulations proposed depend on the range ofvalues prescribed in the simulation process for each input data, theyare modifiable and adjustable to any experimental conditions. 相似文献
18.
The three-dimensional nonlinear quasi-geostrophic potential vorticity equation is reduced to a linear form in the stream function in spherical coordinates for the permanent wave solutions consisting of zonal wavenumbers from 0 to n and rn vertical components with a given degree n. This equation is solved by treating the coefficient of the Coriolis parameter square in the equation as the eigenvalue both for sinusoidal and hyperbolic variations in vertical direction. It is found that these solutions can represent the observed long term flow patterns at the surface and aloft over the globe closely. In addition, the sinusoidal vertical solutions with large eigenvalue G are trapped in low latitude, and the scales of these trapped modes are longer than 10 deg. lat. even for the top layer of the ocean and hence they are much larger than that given by the equatorial β-plane solutions. Therefore such baroclinic disturb-ances in the ocean can easily interact with those in the atmosphere.Solutions of the shallow water potential vorticity equation are treated in a similar manner but with the effective depth H = RT / g taken as limited within a small range for the atmosphere.The propagation of the flow energy of the wave packet consisting of more than one degree is found to be along the great circle around the globe both for barotropic and for baroclinic flows in the atmosphere. 相似文献
19.
Neil R. Viney 《Boundary-Layer Meteorology》1991,56(4):381-393
In unstable conditions, the set of equations defining the aerodynamic resistance to sensible heat transfer, r
a
, cannot be solved analytically. An iterative technique must be used to obtain r
a
exactly, but this is cumbersome and time consuming. In this paper, a new, empirical equation is presented relating the ratio, Q, of the aerodynamic resistances in neutral and unstable conditions, to the bulk Richardson number, Ri
B
. The equation takes the form Q = a + b(–Ri)
c
, where a, b and c are empirical functions of (z – d)/z
om
. This model is shown to predict r
awith a mean absolute error of 0.06 s m–1 over the ranges -15 < Ri
B
< 0 and 10 < (z – d)/z
om
< 2300. Statistical comparison with other equations that have been proposed for r
a
in unstable conditions indicates the superior precision of the model presented here. 相似文献
20.
本文利用一套具有中尺度分辨率的观测资料,对发生在1983年6月下旬的一次长江流域梅雨暴雨过程进行了诊断研究,并比较了该过程的对流降水活跃期和非活跃期的中尺度环境场特征。结果表明,两个时期的动量场存在明显差异,而水热场差异不大,Q1和Q2以及涡度收支也存在明显差异。在降水活跃期（暴雨集中期）,积云对流对能量和涡度的垂直输送有着重要作用;在水热收支中,起主要作用的是垂直输送项,潜热加热基本上为抬升冷却所平衡,水汽的垂直输送是积云对流的主要水汽源;在涡度收支中,低层散度项和扭转项制造正涡度,并通过积云对流向上输送,无论在低层或高层积累的正涡度都被平流非线性过程所耗损。 相似文献