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A narrow beam of alpha particles with kinetic energy T = 600 keV falls normally on a golden foil incorporating n= 1.1x1019 nuclei/cm2. Find the fraction of alpha particles scattered through the angles θ < θ0 = 20°.

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Because of the cosec4θ/2 dependence of the scattering, the number of particles (or fraction) scattered through θ < θ0 cannot be calculated directly. But we can write this fraction as 

P(θ0)=1-Q(θ0)

where Q (θ0) is the fraction of particles scattered through θ ≥ θ0. This fraction has been calculated before and is 

where n here is a number of nuclei/cm2. Using the data we get 

Q = 0.4 

Thus

P(θ0)=0.6

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