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Chapter 13

Q. 13.1

J. L. Black and colleagues* measured the total cross section for the { }^{12} C (\alpha, n)^{15} O reaction at an incident energy of E_{\alpha}=14.6 MeV to be \sigma_{T}=25 mb. If a 1.0-\mu A α-particle beam \left({ }^{4} He ^{++}\right) is incident on a 4.0-mm^2 carbon target of thickness 1.0\mu A (density =1.9 g / cm ^{3}) for one hour, how many neutrons are produced?

Strategy In order to find the number N_{n} of neutrons produced, we find the probability of scattering and multiply it by the number N_{I} of incident α particles: N_{n}=N_{I} P. To find the probability of scattering, we first need to determine n, the number of nuclei/volume, which we established in Equation (4.8):

n=\frac{\rho N_{ A } N_{M}}{M_{g}} \frac{\text { atoms }}{ cm ^{3}} (4.8)

We can calculate the probability of scattering P=n t \sigma [Equation (13.5)], because we can determine n and thickness t, and we are given the cross section σ. Lastly, we determine the number N_{I} of incident α particles from the beam current and time the beam is on the target.

\text { Probability of scattering }=\frac{N_{s} \sigma}{A}=\frac{n t A \sigma}{A}=n t \sigma (13.5)

Step-by-Step

Verified Solution

Some of the values needed are

 

\rho=1.9 g / cm ^{3} \quad N_{ A }=6.02 \times 10^{23} \text { molecules } / mol

 

N_{M}=1 \text { atom/molecule } \quad M_{g}=12 g / mol

 

If we substitute these values in the equation for n, we have

 

\begin{aligned}n=&\left(\frac{1.9 g }{ cm ^{3}}\right)\left(\frac{6.02 \times 10^{23} \text { molecules }}{ mol }\right) \\& \times\left(\frac{1 \text { atom }}{ molecule }\right)\left(\frac{ mol }{12 g }\right) \\=& 9.53 \times 10^{22} \frac{\text { atoms }}{ cm ^{3}}\end{aligned}

 

The probability of scattering can now be determined from Equation (13.5).

 

\begin{aligned}P=n t \sigma=&\left(9.53 \times 10^{22} \text { nuclei } / cm ^{3}\right)\left(1.0 \times 10^{-6} m \right) \\& \times\left(25 \times 10^{-31} m ^{2}\right)\left(10^{6} cm ^{3} / m ^{3}\right) \\=& 2.4 \times 10^{-7}\end{aligned}

 

The number of incident \alpha \text { particles } N_{I} on the target can be determined by the beam current and length of time the beam is on the target.

 

\begin{aligned}N_{I}=&(1.0 \mu A )\left(\frac{10^{-6} C / s }{\mu A }\right)(1.0 h )\left(3600 \frac{ s }{ h }\right) \\& \times\left[\frac{1 \text { alpha } }{2\left(1.6 \times 10^{-19} C \right)}\right] \\=& 1.1 \times 10^{16} \text { alphas }\end{aligned}

 

Note that we have taken the charge of the incident α particles to be +2e.

The ratio of detected neutrons to incident alpha particles \left(N_{n} / N_{I}\right) is the probability P of scattering. We therefore have

 

\begin{aligned}N_{n} &=N_{I} P=N_{I} n t \sigma \\&=\left(1.1 \times 10^{16} \text { alphas }\right)\left(2.4 \times 10^{-7}\right. \text { neutrons/alpha) }\\&=2.6 \times 10^{9} \text { neutrons }\end{aligned}

 

*J. L. Black et al., Nuclear Physics 115, 683 (1968).