rizer.transport.collision_frequency#
Define momentum transfer and energy collision frequency model used by [Mitchner1973].
Notes
\(\nu_{e h}^{(1)}\) is the momentum transfer collision frequency, in s^-1, between electrons and heavy particles (e.g. neutrals, ions), defined in equation (II 5.6) of [Mitchner1973].
\(\bar{\nu_{e h}}^{(1)}\) is the average momentum transfer collision frequency, in s^-1, between electrons and heavy particles (e.g. neutrals, ions), defined in equation (II 6.29) of [Mitchner1973].
\(\nu_{e h}^{E} = \frac{2 m_e}{m_h} \nu_{e h}^{(1)}\) is the energy exchange collision frequency, in s^-1, between electrons and heavy particles (e.g. neutrals, ions), defined in equation (II 7.6) of [Mitchner1973].
\(\bar{\nu_{e h}}^{E}\) is the average energy exchange collision frequency, in s^-1.
Attributes#
Classes#
Module Contents#
- rizer.transport.collision_frequency.logger#
- class rizer.transport.collision_frequency.MomentumTransferCollisionFrequencyModel(name: str, cross_section_model: rizer.transport.cross_sections.MomentumTransferCrossSectionModel)#
- name#
- cross_section_model#
- get_mean_momentum_transfer_collision_frequency(T: float, n_h: float, n_e: float | None = None) float#
Get the mean momentum transfer collision frequency.
- Parameters:
- Returns:
Momentum transfer collision frequency in s^-1.
- Return type:
Notes
The mean momentum transfer collision frequency is defined in equation (II 6.29) of [Mitchner1973] as:
\[\bar{\nu_{e h}}^{(1)} = n_h \bar{Q}_{12} v_{th}\]where:
\(\bar{\nu_{e h}}^{(1)}\) is the average momentum transfer collision frequency,
\(n_h\) is the heavy particle density,
\(\bar{Q}_{12}\) is the mean momentum transfer cross section in m²,
\(v_{th}\) is the electron thermal velocity in m/s.
- class rizer.transport.collision_frequency.IonMomentumTransferCollisionFrequencyModel(name: str, Z: int = 1)#
Bases:
MomentumTransferCollisionFrequencyModel- name#
- Z = 1#
- cst#
- get_mean_momentum_transfer_collision_frequency(T: float, n_h: float, n_e: float | None = None) float#
Get the mean momentum transfer collision frequency.
It is defined in equation (II 8.10) of [Mitchner1973], and assumes that ions are only ionized once. For the case of multiply ionized ions, a factor of \(Z^2\) should be included in the collision frequency expression, where \(Z\) is the ion charge state. See eq. 3.33 in https://www-thphys.physics.ox.ac.uk/people/FelixParra/CollisionalPlasmaPhysics/notes/lecII_electronion.pdf
- Parameters:
Notes
The mean momentum transfer collision frequency for collision between an electron and an ion is defined in equation (II 8.10) of [Mitchner1973] as:
\[\bar{v}_{e i} \equiv n_i \frac{4 \sqrt{2 \pi}}{3}\left(\frac{m_e}{k T}\right)^{3 / 2} \left(\frac{e^2}{4 \pi \epsilon_0 m_e}\right)^2 \ln \Lambda\]where:
\(\bar{\nu_{e h}}^{(1)}\) is the average momentum transfer collision frequency,
\(n_h\) is the heavy particle density,
\(\bar{Q}_{12}\) is the mean momentum transfer cross section in m²,
\(v_{th}\) is the electron thermal velocity in m/s.