Cross section of interaction in recharge model¶
The effective cross section is a physical quantity characterizing the probability of transition of a system of two interacting particles to a certain final state, a quantitative characteristic of the acts of collision of particles of a stream hitting a target with target particles. The effective cross-section has the dimension of the area.
Notation:
\(a_0\) (
a_0
) isbohr_radius
.\(\mathrm{IE}_\text{H}\) (
IE_h
) ishydrogen_ionization_energy
.\(k_\text{B}\) (
k_B
) isboltzmann_constant
.\(e\) (
e
) iselementary_charge
.
- cross_section¶
cross_section
of interaction of particles.
- Symbol:
sigma
- Latex:
\(\sigma\)
- Dimension:
area
- Symbol:
E_i
- Latex:
\(E_\text{i}\)
- Dimension:
energy
- Symbol:
m
- Latex:
\(m\)
- Dimension:
mass
- Symbol:
p
- Latex:
\(p\)
- Dimension:
pressure
- temperature¶
Gas
temperature
.
- Symbol:
T
- Latex:
\(T\)
- Dimension:
temperature
- electric_field_strength¶
- Symbol:
E
- Latex:
\(E\)
- Dimension:
voltage/length
- law¶
sigma = pi * a_0^2 * IE_h / E_i * log(sqrt(3 * k_B * T / m) * sqrt(E_i / IE_h) * sigma * p * m / (2 * k_B * T * e * E))^2
- Latex:
- \[\sigma = \pi a_0^{2} \frac{\mathrm{IE}_\text{H}}{E_\text{i}} \log \left( \sqrt{\frac{3 k_\text{B} T}{m}} \sqrt{\frac{E_\text{i}}{\mathrm{IE}_\text{H}}} \frac{\sigma p m}{2 k_\text{B} T e E} \right)^{2}\]