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Magellan radar scattering from the surface of Venus.

机译:麦哲伦雷达从金星表面散射。

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Magellan spacecraft probed the surface of Venus with 12.6 cm microwave radar over a period of three years. A discretized Fredholm integral equation of the first kind describes the interaction of the altimeter radiation with the surface, and a constrained linear least-squares solution provides estimates of the surface's specific radar backscatter cross section {dollar}sigmasb0(phi){dollar} at incidence angles {dollar}phi{dollar} from {dollar}0spcirc{dollar} to {dollar}6spcirc{dollar}-{dollar}12spcirc{dollar} at over a million surface locations. Linear regularization minimizing the solution's second derivative ensures stability. The resolution of the observations is {dollar}0.5spcirc{dollar}-{dollar}1spcirc{dollar} in {dollar}phi{dollar} and 20-100 km in surface dimension. SAR observations at {dollar}15spcirc{dollar}-{dollar}50spcirc{dollar} yield diffuse cross section measurements. The combined scattering function estimates are organized in a spatial database at 20 km resolution.; The altimeter echo spectrum exhibits Doppler centroid shifts of up to 3 kHz from that expected from a nadir echo. These shifts cannot be attributed to navigational error, pointing error, or measurement uncertainties. Matching Doppler shifts observed by the Venera-16 spacecraft several years earlier and consistent repeat observations by Magellan of the same surface locations demonstrate a surficial origin. Specific structures consistent with the observed shifts include (i) 0.01-1 km-scale tilts of up to {dollar}1spcirc{dollar} and (ii) sudden changes in surface reflectivity {dollar}rho.{dollar} Other possible causes, such as anisotropic scattering due to 0.1-1 m-scale surface features, are postulated but not conclusively identified.; The form of the scattering function {dollar}sigmasb0(phi){dollar} varies substantially with location. Least-squares fits to three standard scattering models, Hagfors, Gaussian, and exponential, show that no single model of this type is consistent with all the observations. Overall, the exponential model fits best in plains regions and the Gaussian model fits best in complex tesserae, while the Hagfors model gives best agreement only in limited areas, typically the smoothest regions. Random surface profiles having the same height distribution and correlation functions but different slope distribution functions demonstrate that the human eye is sensitive to correlation length while the coherent radar is sensitive to slope distribution.
机译:麦哲伦号航天器在三年内用12.6 cm微波雷达探测了金星表面。第一种离散化的Fredholm积分方程描述了高度计辐射与表面的相互作用,并且受约束的线性最小二乘解提供了入射时表面特定雷达后向散射截面{dollar} sigmasb0(phi){dollar}的估计值在超过一百万个表面位置上,从{美元} 0spcirc {dollar}到{dollar} 6spcirc {dollar}-{dollar} 12spcirc {dollar}的角度{dollar} phi {dollar}线性正则化最小化了解决方案的二阶导数,从而确保了稳定性。观测的分辨率为{dol} phi {dollar}为{splar} 0.5spcirc {dollar}-{dollar} 1spcirc {dollar},表面尺寸为20-100 km。在$ 15spcirc {dollar- $ 50spcirc {dollar}的SAR观测值可得出散射截面测量结果。组合的散射函数估计值以20 km的分辨率组织在空间数据库中。高度计回波频谱显示出比最低点回波所期望的多普勒质心偏移高达3 kHz。这些变化不能归因于导航误差,指向误差或测量不确定性。几年前Venera-16航天器观测到的匹配多普勒频移以及麦哲伦对相同表面位置的一致重复观测表明是表面原因。与观察到的偏移一致的特定结构包括(i)0.01-1 km尺度的倾斜度,最高可达{sp} {sp},以及(ii)表面反射率突然变化。{r}。其他可能的原因,例如假设由于0.1-1 m尺度的表面特征而产生的各向异性散射,但并未最终确定。散射函数{sigmasb0(phi){dollar}的形式随位置而变化。最小二乘拟合三个标准散射模型(Hagfors,高斯和指数),表明没有一个这种类型的模型与所有观测值一致。总体而言,指数模型最适合于平原地区,而高斯模型最适合于复杂的镶嵌物体,而Hagfors模型仅在有限的区域(通常是最光滑的区域)具有最佳一致性。具有相同的高度分布和相关函数但斜率分布函数不同的随机表面轮廓表明,人眼对相关长度敏感,而相干雷达对斜率敏感。

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