Classical Electrodynamics |
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9.10 Scattering by a Conducting Sphere in the Short-Wavelength Limit Another
type of problem which is essentially diffraction is the scattering of waves by an
obstacle. We will consider the scattering of a plane electromagnetic wave by a ...
9.10 Scattering by a Conducting Sphere in the Short-Wavelength Limit Another
type of problem which is essentially diffraction is the scattering of waves by an
obstacle. We will consider the scattering of a plane electromagnetic wave by a ...
Page
The multiple-scattering distribution for the projected angle of scattering | In (
210ZT*) t (13.111) 1S 1 62 PM (6') d6' = — exp (— #) d6' (13.112) M Vr(0°) (0°)
where both positive and negative values of 6' are considered. The smallangle ...
The multiple-scattering distribution for the projected angle of scattering | In (
210ZT*) t (13.111) 1S 1 62 PM (6') d6' = — exp (— #) d6' (13.112) M Vr(0°) (0°)
where both positive and negative values of 6' are considered. The smallangle ...
Page
13.8 Multiple and single scattering distributions of projected angle. In the region
of plural scattering (x > 2–3) the dotted curve indicates the smooth transition from
the small-angle multiple scattering (approximately Gaussian in shape) to the ...
13.8 Multiple and single scattering distributions of projected angle. In the region
of plural scattering (x > 2–3) the dotted curve indicates the smooth transition from
the small-angle multiple scattering (approximately Gaussian in shape) to the ...
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Contents
Introduction to Electrostatics | 1 |
Nš 3 | 3 |
Greens theorem | 14 |
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