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Approximation of single scattering properties of ice and snow particles for high microwave frequencies

机译:高微波频率下冰和雪颗粒的单次散射特性的近似值

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As satellite high-frequency passive microwave data have recently become available, there is an increasing demand for an accurate and computationally efficient method to calculate the single scattering properties of nonspherical ice particles, so that it may be used in radiative transfer models for physical retrievals of ice water path and snowfall rate. In this study, two such approximations are presented for calculating the single scattering properties of three types of large ice particles: bullet rosettes, sector snowflakes, and dendrite snowflakes, for the frequency range of 85 to 220 GHz, based on results of discrete-dipole approximation (DDA) modeling. By analyzing the DDA modeling results, it is noted that, for nonspherical ice particles, the scattering and absorption cross sections and the asymmetry parameter have a magnitude between those of the two imaginary equal-mass spheres. One is a solid sphere, and the other is an ice-air mixed soft sphere whose diameter equals the particle's maximum dimension. Therefore, the first approximation involves substituting the single scattering properties of a nonspherical ice particle with those of an equal-mass sphere, which can be calculated by Lorenz-Mie theory, with an effective dielectric constant derived by mixing ice and air using the Maxwell-Garnett formula. The diameter of such an equal-mass sphere D is bigger than the diameter of the solid sphere D-0, but smaller than the particle's maximum dimension D-max. Defining a softness parameter SP = (D-D-0)/(Dmax-D0), it is found that the best-fit equal-mass sphere has an SP value of 0.2 similar to 0.5 for calculating the volume scattering coefficient, depending on frequency and particle shape. At 150 GHz, the best-fit softness parameter is found to be similar to 1/3 when averaging over all particle shapes. For calculating the asymmetry parameter, the DDA model results show that the best-fit softness parameter is close to 0 (i.e., the same as the solid sphere) for frequencies higher than 150 GHz, while it is about 0.3 for 85.5 GHz. The second approximation presented is a polynomial fit to the scattering and absorption cross sections and the asymmetry parameter using the particle size parameter as an independent variable. For the scattering cross section, three fitting curves are derived for, respectively, rosettes, sector snowflakes, and dendrite snowflakes. For the absorption cross section, a single curve is used to fit all particle shapes. For the asymmetry parameter, two curves are derived, one for rosettes and one for snowflakes. The best-fit softness parameter for three particular frequencies ( 85.5, 150, and 220 GHz) and for three particle shapes in the first approximation, as well as the coefficients of the polynomial fit in the second approximation, are presented. After implementing these approximations in a radiative transfer model, radiative transfer simulations are carried out for a snowfall and an ice cloud case. The simulated brightness temperatures based on the two approximations agree with each other within 3 K, but are significantly different from those based on the solid- and the soft-sphere approximations.
机译:随着近来卫星高频无源微波数据的可用,对计算非球形冰粒单个散射特性的精确且计算效率高的方法的需求日益增长,因此可以将其用于辐射传递模型中以进行物理取回。冰水路径和降雪率。在这项研究中,基于离散偶极子的结果,提出了两种近似方法来计算三种大冰粒(子弹玫瑰,扇形雪花和树枝状雪花)在85至220 GHz频率范围内的单散射特性。近似(DDA)建模。通过分析DDA建模结果,可以注意到,对于非球形冰粒,散射和吸收截面以及不对称参数的大小介于两个假想的等质量球的大小之间。一个是实心球,另一个是冰-空气混合软球,其直径等于粒子的最大尺寸。因此,第一近似方法是将非球形冰粒的单个散射特性替换为等质量球体的单个散射特性(可以通过Lorenz-Mie理论计算得出),并使用有效的介电常数,该常数是使用麦克斯韦-加内特公式。这样的等质量球D的直径大于实心球D-0的直径,但小于粒子的最大尺寸D-max。定义柔软度参数SP =(DD-0)/(Dmax-D0),可以发现最佳拟合等质量球的SP值为0.2,类似于0.5,用于计算体积散射系数,具体取决于频率和颗粒形状。在150 GHz时,对所有粒子形状求平均时,最佳拟合柔软度参数类似于1/3。为了计算不对称参数,DDA模型结果表明,对于高于150 GHz的频率,最佳拟合软度参数接近0(即与实心球相同),而对于85.5 GHz则为0.3。给出的第二个近似值是使用粒径参数作为自变量对散射截面和吸收截面以及不对称参数的多项式拟合。对于散射横截面,分别针对玫瑰花结,扇形雪花和枝状雪花得出了三个拟合曲线。对于吸收截面,使用一条曲线来拟合所有颗粒形状。对于不对称参数,导出了两条曲线,一条曲线用于玫瑰花结,一条曲线用于雪花。给出了三个特定频率(85.5、150和220 GHz)的最佳拟合软度参数以及在第一近似中的三种粒子形状的最佳拟合软度参数,以及在第二近似中的多项式拟合系数。在辐射传递模型中实现了这些近似值之后,针对降雪和冰云情况进行了辐射传递模拟。基于两个近似值的模拟亮度温度在3 K内彼此一致,但与基于实球和软球近似值的模拟亮度温度存在显着差异。

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