Example 4.8
Find the fraction of a beam of 7.7-MeV alpha particles that is scattered through angles of more
than 45° when incident upon a gold foil 3 10 ^7 m thick. These values are typical of the alpha-
particle energies and foil thicknesses used by Geiger and Marsden. For comparison, a human
hair is about 10^4 m in diameter.
Solution
We begin by finding n, the number of gold atoms per unit volume in the foil, from the relationship
n
Since the density of gold is 1.93 104 kg/m^3 , its atomic mass is 197 u, and 1 u 1.66
10 ^27 kg, we have
n
5.90 1028 atoms/m^3
The atomic number Zof gold is 79, a kinetic energy of 7.7 MeV is equal to 1.23 10 ^12 J,
and 45°; from these figures we find that
f 7 10 ^5
of the incident alpha particles are scattered through 45° or more—only 0.007 percent! A foil
this thin is quite transparent to alpha particles.
In an actual experiment, a detector measures alpha particles scattered between
and d, as in Fig. 4.33. The fraction of incident alpha particles so scattered is
found by differentiating Eq. (4.31) with respect to , which gives
1.93 104 kg/m^3
(197 u/atom)(1.66 10 ^27 kg/u)
massm^3
massatom
atoms
m^3
156 Appendix to Chapter 4
Figure 4.33In the Rutherford experiment, particles are detected that have been scattered between
and d.
Foil
dθ
θ
r r sin θ
rdθ
Area = 4πr^2 sin cos θ 2 2 θdθ
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