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首页> 外文期刊>Atmospheric chemistry and physics >Microphysical properties of frozen particles inferred from Global Precipitation Measurement (GPM) Microwave Imager (GMI) polarimetric measurements
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Microphysical properties of frozen particles inferred from Global Precipitation Measurement (GPM) Microwave Imager (GMI) polarimetric measurements

机译:从全球降水量测量(GPM)微波成像仪(GMI)极化测量推断出的冷冻颗粒的微物理性质

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Scattering differences induced by frozen particle microphysical properties are investigated, using the vertically (V) and horizontally (H) polarized radiances from the Global Precipitation Measurement (GPM) Microwave Imager (GMI) 89 and 166?GHz channels. It is the first study on frozen particle microphysical properties on a global scale that uses the dual-frequency microwave polarimetric signals.brbrFrom the ice cloud scenes identified by the 183.3?±?3?GHz channel brightness temperature (iT/isubb/sub), we find that the scattering by frozen particles is highly polarized, with V–H polarimetric differences (PDs) being positive throughout the tropics and the winter hemisphere mid-latitude jet regions, including PDs from the GMI 89 and 166?GHz TBs, as well as the PD at 640?GHz from the ER-2 Compact Scanning Submillimeter-wave Imaging Radiometer (CoSSIR) during the TC4 campaign. Large polarization dominantly occurs mostly near convective outflow regions (i.e., anvils or stratiform precipitation), while the polarization signal is small inside deep convective cores as well as at the remote cirrus region. Neglecting the polarimetric signal would easily result in as large as 30?% error in ice water path retrievals. There is a universal qbell curve/q in the PD–TBsubV/sub relationship, where the PD amplitude peaks at ?~??10?K for all three channels in the tropics and increases slightly with latitude (2–4?K). Moreover, the 166?GHz PD tends to increase in the case where a melting layer is beneath the frozen particles aloft in the atmosphere, while 89?GHz PD is less sensitive than 166?GHz to the melting layer. This property creates a unique PD feature for the identification of the melting layer and stratiform rain with passive sensors.brbrHorizontally oriented non-spherical frozen particles are thought to produce the observed PD because of different ice scattering properties in the V and H polarizations. On the other hand, turbulent mixing within deep convective cores inevitably promotes the random orientation of these particles, a mechanism that works effectively in reducing the PD. The current GMI polarimetric measurements themselves cannot fully disentangle the possible mechanisms.
机译:使用全球降水量测量(GPM)微波成像仪(GMI)89和166?GHz通道的垂直(V)和水平(H)极化辐射,研究了由冷冻颗粒微物理特性引起的散射差异。这是首次使用双频微波极化信号在全球范围内对冷冻粒子的微物理性质进行研究。 从183.3?±?3?GHz通道亮度温度(< i> T b ),我们发现冻结粒子的散射是高度极化的,整个热带和冬季半球的V–H极化差异(PDs)为正TC4战役期间,包括来自GMI 89和166?GHz TB的局部放电以及ER-2紧凑型扫描亚毫米波成像辐射计(CoSSIR)产生的640?GHz局部放电。大极化主要发生在对流流出区域附近(即,砧或层状降水),而极化信号在深对流岩心内部以及偏远的卷云区域较小。忽略极化信号将很容易导致在冰水路径检索中产生高达30%的误差。 PD-TB V 关系中存在一条通用的钟形曲线,其中,热带地区所有三个通道的PD幅值均在?〜?? 10?K处达到峰值并增加稍有纬度(2-4?K)。此外,在融化层位于大气中高空冻结颗粒之下的情况下,166?GHz PD趋于增加,而89?GHz PD对融化层的敏感性不如166?GHz。此属性创建了独特的PD特性,可通过被动传感器识别融化层和层状雨。 由于V中的冰散射特性不同,水平定向的非球形冻结粒子被认为可产生观察到的PD。和H极化。另一方面,深对流核内的湍流混合不可避免地促进了这些粒子的无规取向,这种机制有效地降低了PD。当前的GMI极化测量本身无法完全解开可能的机制。

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