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NOTE: DirectCast and TryCast provide somewhat better performance than CType when you re converting from the Object data type to a more specific data type

10-6

Scattering Angle (Degrees)

Scattering Angle (Degrees)

Figure 5.1.5 (a) Close to grazing angle and composite surface. Incident angle (}i = 85 , 9 = 0.125L, b = 400. hI = 0.1A, and h = 0.3.\, h2 = 0.5.\, and 12 = 5-\ for one realization. (b) Close to grazing angle and composite surface. Averaged over 50 realizations. (c) Comparison near-backscattering angle for various surface lengths. Parameters are those of (a). For 2500 wavelengths surface 50 realizations of Fig. 5.1.5b is used and others are averaged over 10 realizations. The bandwidths of L = 200.\ and L = 800.\ are the same as Fig. 5.1.4a, for L = 400.\, b = 300(30.\). (d) Comparison near-backscattering angle with the periodic boundary condition method (PBC). For BMIA/CAG the result of (b) is used. The PBC is for the surface length of 40 wavelengths and averaged over 30 realizations. Parameters are those of (a).

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DirectCast casts a variable from a de ned type to a more specialized type in the same object hierarchy TryCast is similar to DirectCast, but it doesn t fail if the operation is unsuccessful Instead, it returns Nothing You can use the DirectCast and TryCast keywords only when casting from a general type to a more speci c type, such as from type Object to type Control or, even more speci cally, to type TextBox The cast type must be in the same object hierarchy as the original type So you can use these keywords to cast from a variable declared as a general Object data type to a Control data type, because a control is an object, but you cannot use them to cast from a String data type to an Integer data type, because an integer is not a string Cast a variable from an object type to a more speci c type as follows:

Figure 5.1.6 Magnitude of the surface current for one realization for the PBC method with P = 40 wavelengths. Parameters are those of Fig. 5.1.5a.

In the application of the method of moments to the rough surface scattering problem, a common implementation is to use a grid of 10 points per free-space wavelength to discretize the surface. We shall call such a gridding a single coarse grid (SCG). However, in lossy dielectric surfaces, the wavelength in the dielectric medium is much shorter. Thus in scattering by lossy dielectric rough surfaces with high permittivity, there can be rapid spatial variation of surface fields. For microwave remote sensing applications, both wet soil surfaces and ocean surfaces can have large permittivity. Two alternatives were used. The first alternative is to use impedance boundary condition as shown in 4. The disadvantage of this alternative is that an approximation is used in the problem. The second alternative is to use a dense grid with a large number of points (say more than 30 points) per free-space wavelength. We shall call such a gridding a single dense grid (SDG). We have shown in 4 that dense sampling of points is a requirement for energy conservation and an accurate calculation of emissivity. The disadvantage of this second alternative is that there is a large increase in CPU and required memory. The physics-based two-grid (PBTG) method to be discussed in this section is an improvement over these two alternatives in that it has the same accuracy as the single dense grid and yet has a CPU comparable with that of the single coarse grid. To demonstrate the accuracy of the PBTG method, we use it to calculate the emissivity of a random rough surface. In PBTG, two grids were used: a dense grid and a sparse grid. The

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