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File:Radar cross section of metal sphere from Mie theory.svg

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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).
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Author Catslash

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27 June 2009

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Date/TimeThumbnailDimensionsUserComment
current18:06, 24 April 2010Thumbnail for version as of 18:06, 24 April 2010640 × 480 (90 KB)Catslashrm spurious white rectangle at top left
01:09, 6 July 2009Thumbnail for version as of 01:09, 6 July 2009640 × 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 2009Thumbnail for version as of 16:01, 27 June 2009640 × 480 (88 KB)Catslash
01:36, 27 June 2009Thumbnail for version as of 01:36, 27 June 2009512 × 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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