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Rayleigh scatterer

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Rayleigh scatterer
[rā′lē]
Etymology: John W.S. Rayleigh, English physicist, 1842-1919
reflecting objects whose dimensions are much smaller than the ultrasonic wavelength. The scattered intensity from a volume of Rayleigh scatterers increases rapidly with increasing frequency, being related to frequency raised to the fourth power.


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If the light scattering is due to well-defined scatterers, then the total cross section [Sigma] of the scatterer, the number [Rho] of scatterers per unit volume and the scattering mean free path L yield: [Sigma] = [integral of] [d[Sigma]([Omega])/d[Omega]] d[Omega] (2) and L = 1/[Rho][Sigma] (3) A scatterer having a radius r much smaller than the wave length [Lambda] in the medium is a Rayleigh scatterer and its total cross section yields [Mathematical Expression Omitted] (4) where [n.
 
 
 
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