Numerical Evaluation of Planetary Radar Backscatter Models for Self-Affine Fractal Surfaces

被引:1
|
作者
Virkki, Anne [1 ,2 ]
机构
[1] Univ Helsinki, Dept Phys, Gustaf Hallstrominkatu 2, Helsinki 00560, Finland
[2] Finnish Geospatial Res Inst, Natl Land Survey, Vuorimiehentie 5, Espoo 02150, Finland
关键词
radar; microwave scattering; fractal surfaces; planetary science; SHAPE MODEL; SCATTERING; ROUGHNESS; TOPOGRAPHY;
D O I
10.3390/rs16050890
中图分类号
X [环境科学、安全科学];
学科分类号
08 ; 0830 ;
摘要
Numerous analytical radar-scattering laws have been published through the past decades to interpret planetary radar observations, such as Hagfors' law, which has been commonly used for the Moon, and the cosine law, which is commonly used in the shape modeling of asteroids. Many of the laws have not been numerically validated in terms of their interpretation and limitations. This paper evaluates radar-scattering laws for self-affine fractal surfaces using a numerical approach. Traditionally, the autocorrelation function and, more recently, the Hurst exponent, which describes the self-affinity, have been used to quantify the height correlation. Here, hundreds of three-dimensional synthetic surfaces parameterized using a root-mean-square (rms) height and a Hurst exponent were generated, and their backscattering coefficient functions were computed to evaluate their consistency with selected analytical models. The numerical results were also compared to empirical models for roughness and radar-scattering measurements of Hawaii lava flows and found consistent. The Gaussian law performed best at predicting the rms slope regardless of the Hurst exponent. Consistent with the literature, it was found to be the most reliable radar-scattering law for the inverse modeling of the rms slopes and the Fresnel reflection coefficient from the quasi-specular backscattering peak, when homogeneous statistical properties and a ray-optics approach can be assumed. The contribution of multiple scattering in the backscattered power increases as a function of rms slope up to about 20% of the backscattered power at normal incidence when the rms slope angle is 46 degrees.
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页数:30
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