b)
Students want to carry out an investigation into gamma photon absorption using a source of
.
They add sheets of lead between the source
S and a radiation detector
T, to give a total thickness
d of lead.
S and
T remain in fixed positions, as shown in Fig. 2.1.
Fig. 2.1
i)
The
source emits beta radiation as well as gamma radiation.
Explain why this would not affect the experiment.
[1]
ii)
The students record the number N of gamma photons detected by T in 10 minutes for each different thickness d of lead. The background count is negligible.
The results are shown in a table. The table includes values of ln N, including the absolute uncertainties.
N |
d/mm |
ln N |
4300 ± 440 |
0 |
8.37 ± 0.10 |
2500 ± 250 |
10 |
7.82 ± 0.10 |
1400 ± 150 |
20 |
7.24 ± 0.11 |
800 ± 90 |
30 |
6.68 ± 0.11 |
500 ± 60 |
40 |
6.21 ± 0.12 |
300 ± 40 |
50 |
|
N and d are related by the equation N = N0 e–μd where N0 and μ are constants.
1.
The students decide to plot a graph of ln N against d.
Show that this should give a straight line with gradient
= – μ and y-intercept = ln N0.
[1]
2.
Complete the missing value of ln N in the table, including the absolute uncertainty.
Show your calculation of the absolute uncertainty in the space below.
[2]
3.
In Fig. 2.2, five of the data points have been plotted, including error bars for ln N.
- Plot the missing data point and error bar.
- Draw a straight line of best fit and one of worst fit.
[2]
Fig. 2.2
4.
Use Fig. 2.2 to determine the value of μ in m–1, including the absolute uncertainty.
μ = ...................... ± ...................... m–1 [4]
5.
Determine the thickness, d1⁄2, of lead which halves the number of gamma photons reaching T.
d1⁄2 = ........................................ m [2]