Showing posts with label Scattering cross section. Show all posts
Showing posts with label Scattering cross section. Show all posts

Nuclear & Particle Physics - Scattering cross section

A proton beam is incident on a scatterer 0.1 centimeter thick. The scatterer contains 1020 target nuclei per cubic centimeter. In passing through the scatterer, one proton per incident million is scattered. The scattering cross section is 

A. 10−29 cm²
B. 10−27 cm²
C. 10−25 cm²
D. 10−23 cm²
E. 10−21 cm²
(GR8677 #42 )
Solution:

Given:
Thickness: T = 10−1 cm
Density: ρ = N/V = 1020 nuclei/cm³
Number of proton per incident million: N = 10−6

The scattering cross section → Area A = Volume/Thickness
A = V/T =  (V/N) × (N/T) = (1/ρ) × (N/T) = N/ρT
A = 10−6 / (1020 × 10−1) = 10−6−20+1 = 10−25 cm²

Answer: C

Nuclear & Particle Physics – Scattering cross section

A beam of 1012 protons per second is incident on a target containing 1020 nuclei per square cm. At an angle of 10 degrees, there are 102 protons per second elastically scattered into a detector that subtends a solid angle of 10−4 steradians. What is the differential elastic scattering cross section, in units of sq cm per steradian?

A. 1024
B. 1025
C. 1026
D. 1027
E. 1028
(GR9277 #95)
Solution:

Using dimension analysis:

the fractional scattering rate:



In units of sq cm per steradian:



Answer: C