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Summary
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| Description |
English: Monostatic radar cross section (RCS) of a perfectly conducting metal sphere as a function of frequency (computed by Mie theory). The x-axis is the relative frequency, defined as the number of wavelengths in the circumference, and equal to the wavenumber times the radius i.e. frel = 2πR/λ = kR. The y-axis is the RCS relative to the projected area of the sphere i.e. σ/(πR2). The asymptotes are σ/(πR2) = 9 (frel)4 in the low frequency (Rayleigh) region (λ > 2πR) , and σ/(πR2) = 1 in the high frequency (optical) limit (λ << R). |
| Date | |
| Source | Own work |
| Author | Catslash |
Licensing
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I, the copyright holder of this work, release this work into the public domain. This applies worldwide. In some countries this may not be legally possible; if so: I grant anyone the right to use this work for any purpose, without any conditions, unless such conditions are required by law. |
File history
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| Date/Time | Thumbnail | Dimensions | User | Comment | |
|---|---|---|---|---|---|
| current | 18:06, 24 April 2010 | | 640 × 480 (90 KB) | Catslash | rm spurious white rectangle at top left |
| 01:09, 6 July 2009 |  | 640 × 480 (92 KB) | Catslash | {{Information |Description={{en|1=Monostatic radar cross section [RCS] of a perfectly conducting metal sphere as a function of frequency (computed by Mie theory). The x-axis is the relative frequency, defined as the number of wavelengths in the circumfere | |
| 16:01, 27 June 2009 |  | 640 × 480 (88 KB) | Catslash | ||
| 01:36, 27 June 2009 |  | 512 × 512 (88 KB) | Catslash | {{Information |Description={{en|1=Monostatic radar cross section [RCS] of a perfectly conducting metal sphere as a function of frequency (computed by Mie theory). The x-axis is the relative frequency, defined as the number of wavelengths in the circumfere |
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