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