Ekman动量近似下中间边界层模式中的风场结构

发展了一个准三维的、中等复杂的边界层动力学模式，该模式包含了EKman动量近似下的惯性加速度和Blackadar的非线性湍流粘性系数，它进一步改进了Tan和Wu(1993）提出的边界层理论模型。该模型在数值计算复杂性上与经典Ekman模式相类似，但由于包含了Ekman动量近似下的惯性项，使得该模式比传统Ekman模式更近于实际过程。中详细地比较了该模式与其他简化边界层模式在动力学上的差异，结果表明：在经典的Ekman模式中，由于忽略了流动的惯性项作用，导致在气旋性切变气流（反气旋性切变气流）中风速和边界层顶部的垂直速度的高估（低估），而在半地转边界层模式中，由于高估了流动惯性项的作用，结果与经典Ekman模式相反。同样，该模式可以应用于斜压边界层，对于Ekman动量下的斜压边界层风场同时具有经典斜压边界层和Ekman动量近似边界层的特征。     

风廓线雷达大气风场观测误差分析

依据风廓线雷达工作原理和风的计算公式,分析影响大气风场观测误差的主要因素,重点分析了雷达回波SNR对风的观测精度影响和GPS探空对比试验。结果表明:①风速观测精度主要取决于波束倾角、雷达技术参数和大气折射率结构常数C2n的垂直分布;风速及风速观测精度越大,风向观测精度越大。②在同种观测模式下,波束倾角与C2n越大,风场观测精度越高。③同一观测模式的SNR越大,风速观测误差越小;不同模式间的大气风场观测精度相差较大。④对比试验的风速风向相关性较好,但相对偏差较大,尤其低空更为明显。     

Relating Urban Surface-layer Structure to Upwind Terrain for the Salford Experiment (Salfex)

Profiles of wind and turbulence over an urban area evolve with fetch in response to surface characteristics. Sodar measurements, taken on 22 April 2002 during the Salford Experiment in the UK (Salfex), are here related to upstream terrain. A logarithmic layer up to z = 65m was observed in all half-hour averaged profiles. Above this height the profile showed a different vertical gradient, suggesting a change in surface cover upstream. The drag coefficient varied by a factor of two over only a 20° direction change. Turbulence intensity (σ _x ) for each wind component (x) decreased with height, but the ratio suggested an underestimate of σ _u compared to previous results. Mean urban and suburban cover fraction within the source area for each height decreased sharply between z = 20 and 50m, increasing slightly above. The near-convergence of cover fractions thus occured for source areas of minimum length ≈ 2,200 m. In comparison, the mean length scale of heterogeneity L _P was calculated from surface cover data to be 1,284 m, and the corresponding mean blending height h _b was 175 m. Finally, the mean streamline angle, α, was negative and the magnitude decreased with height. An exponential fit to α for z ≤ 65m gave an e-folding height scale of 159 m. A simple relationship between this height scale and L _P was assumed, giving L _P ≈ 1,080 m, which is in reasonable agreement with the estimate from surface cover type. The results suggest that more emphasis is required on modelling and measuring surface-layer flow over heterogeneous urban canopies.     

投弃式海流剖面测量仪测量原理研究

根据投弃式海流剖面测量仪的测量原理建立了二维海流运动感生电场离散和连续模型,通过模型推导得到了海流与感生电场间的关系公式。通过对海流感生电磁场的分析,对海流测量的基本方法进行了研究,通过感生电磁场的量级的计算,确定了投弃式海流剖面测量仪研究的主要方向和关键技术。     

Near-Wall Flow Development After A Step Change In Surface Roughness

An experimental study of the initial flow field downstream of a step change in surface roughness is presented. The roughness length of the downstream surface was approximately tenfold that of the upstream roughness and, unlike all previous studies, attention was concentrated on the roughness sublayer region beneath the inertial (log-law) region. The experiments were conducted at a boundary layer Reynolds number of about 6 × 10⁴ (based on layer thickness andfree-stream velocity) and around a longitudinal location where the (downstream) roughness length, z_o2, was about 1% of the boundary-layer thickness atthe roughness change point.The thickness of the roughness sublayer was found for the two roughness. It was observed that the vertical profiles of mean velocity and turbulence characteristics started to show similarity after about 160z₀₂ downstream of the roughness change. The presence of a shear stress overshoot is shown to depend strongly on the precise location (with respect to the roughness elements) at which the measurements are made and the thickness of the equilibrium layer is shown to be very sensitive to the way it is defined. It is demonstrated that the growing equilibrium layer has first to encompass the roughness sublayer before any thickness of inertial sublayer can be developed. It follows that, in somepractical cases, like flows across some urban environments, the latter(log-law) region may never exist at all.     

海浪周期关系的研究

本文利用现场观测数据、实验室风浪槽观测数据和由文氏谱及JONSWAP谱生成的模拟数据,研究了有效周期与谱平均周期、谱峰周期与谱平均周期以及有效周期与谱峰周期的关系,通过数据拟合给出了相应的关系式.研究发现,有效周期与由谱的负阶矩计算的平均周期之间的关系更加稳定,并且有效周期与负2阶矩计算的平均周期几乎相等,均代表了海浪主导波对海浪平均周期的贡献.     

闽北地区边界层移动风廓线雷达对比试验评估

为了更好地把握风廓线雷达的探测性能和数据精度,对移动风廓线雷达与L波段探空雷达资料进行对比统计分析,结果表明：移动风廓线雷达的有效数据获取率达到80％的高度为3500m,符合边界层风廓线雷达的有效探测高度。移动风廓线的径向速度平均差和标准差随着高度的增加而增加,东西方向的径向速度误差比南北方向的高约0．5—1．0m／s。风廓线雷达自身数据的准确性良好,但是降雨对数据的准确性影响比较大。这次对比试验结果表明,对比试验应该选择比较平稳的天气过程。由于秋冬季节大气环流比较稳定,降雨类型多为层状云降雨,因而风廓线雷达数据可靠性高;对流性降雨过程往往造成风廓线雷达资料可靠性降低。     

宜春地区三类典型天气的风廓线雷达产品特征分析

选取江西省宜春市晴空、弱降水、强降水三类天气过程个例,结合天气形势、雷达回波、气象要素等资料,对比分析了风廓线雷达产品特征。结果表明：（1）在晴空天气背景下,风廓线雷达探测高度低,水平风速小,垂直风速正负值交替出现,大气折射率结构常数（Cn2）值最小。（2）在稳定性弱降水天气背景下,大气呈稳定状态,风廓线雷达探测高度随降水的产生而逐渐抬升,高低层有明显的风速切变,850 hPa赣南至赣东北有西南急流穿过,赣北有切变线存在,利于降水产生,垂直风速因降水影响出现朝向雷达正速度,Cn2值比晴空时大。（3）在具有产生强对流天气背景下,大气中对流强烈,风廓线雷达的水平风速增大,西南急流深厚且不断下沉,850-700 hPa有强烈的垂直切变,动力条件和水汽条件利于强降水产生,垂直风速表现为更大的朝向雷达正速度,Cn2值比弱降水时的大。     

风廓线雷达资料在一次强对流天气过程中的应用

通过分析2010年6月28日广州市南沙区强对流天气过程的风廓线雷达资料发现：风廓线雷达测得的温度廓线资料可以很直观地显示边界层逆温及高温区域随时间的变化;风廓线雷达产品（垂直速度和信号噪声比）能清楚地反映降水的开始、结束以及降水的强度;风廓线雷达可以很好的监测到低空急流的发生发展及水平风的垂直切变．对强对流天气的预报有...     

2015年11月沈阳地区一次PM2.5重污染过程综合分析

利用多源观测资料综合分析了2015年11月沈阳地区一次PM2.5 重污染天气的气象条件、垂直风场演变、大气边界层特征以及污染物的来源。结果表明:本次重污染过程中,沈阳市区PM2.5浓度长达81h超过250μg · m^-3 ,其中峰值浓度达到1287μg · m^-3 ,重污染期间PM2.5 /PM10 的比例最高为90%。受地面倒槽和黄淮气旋影响,近地面层持续存在的逆温层、高相对湿度和弱偏北风为颗粒物吸湿增长和长时间聚集提供有利的天气条件。风廓线雷达风场资料显示在重污染期间,近地面层存在弱风速区、凌乱风场和弱下沉气流。利用风廓线雷达资料计算了边界层通风量(Ventilation Index,VI)和局地环流指数(Recirculation,R),边界层通风量VI和PM2.5 存在明显的负相关,非污染日VI是重污染日的2倍,局地环流指数R在重污染天气前大于0.9,而在污染期间部分空间R小于0.8。通过后向轨迹模式和火点监测资料分析发现,沈阳上空300m高度气团来自于生物质燃烧区域,而且沈阳地区NO2和CO浓度的变化与PM2.5一致,说明本次重污染过程也可能和生物质燃烧有关。