Askiitians Tutor Team
Last Activity: 10 Days ago
To find the Coulombic barrier for the penetration of the 90Th232 nucleus by a proton and an alpha particle, we need to understand the concept of the Coulomb barrier. This barrier arises due to the electrostatic repulsion between charged particles, such as protons and alpha particles, and the positively charged nucleus they are approaching. The height of this barrier can be calculated using the principles of electrostatics.
Coulomb Barrier Basics
The Coulomb barrier can be described by the formula:
V = (Z1 * Z2 * e^2) / r
Where:
- V is the potential energy of the Coulomb barrier.
- Z1 is the atomic number of the incoming particle.
- Z2 is the atomic number of the target nucleus.
- e is the elementary charge (approximately 1.6 x 10^-19 coulombs).
- r is the distance of closest approach, often approximated as the sum of the radii of the two nuclei.
Calculating for a Proton
For a proton approaching the 90Th232 nucleus:
- Z1 (proton) = 1
- Z2 (Thorium) = 90
- r can be estimated using the formula: r = r0 * (A1^(1/3) + A2^(1/3)), where A is the mass number. For Thorium, A = 232, and for the proton, A = 1. The constant r0 is approximately 1.2 fm (femtometers).
Calculating r:
r = 1.2 fm * (232^(1/3) + 1^(1/3)) ≈ 1.2 fm * (6.13 + 1) ≈ 8.16 fm
Now substituting into the Coulomb barrier formula:
V = (1 * 90 * (1.6 x 10^-19)^2) / (8.16 x 10^-15)
Calculating this gives:
V ≈ 1.77 MeV
Calculating for an Alpha Particle
Now, let’s calculate the Coulomb barrier for an alpha particle:
- Z1 (alpha particle) = 2
- Z2 (Thorium) = 90
Using the same approach for r:
r = 1.2 fm * (232^(1/3) + 4^(1/3)) ≈ 1.2 fm * (6.13 + 1.59) ≈ 9.12 fm
Now substituting into the Coulomb barrier formula:
V = (2 * 90 * (1.6 x 10^-19)^2) / (9.12 x 10^-15)
Calculating this gives:
V ≈ 2.96 MeV
Summary of Results
In summary, the Coulombic barriers for the penetration of the 90Th232 nucleus are:
- For a proton: approximately 1.77 MeV
- For an alpha particle: approximately 2.96 MeV
These values indicate that the alpha particle faces a higher Coulomb barrier due to its greater charge, making it less likely to penetrate the nucleus compared to a proton, which has a lower charge and thus experiences less repulsion.