permittivity_1D_Maxwellian
- plasmapy.formulary.dielectric.permittivity_1D_Maxwellian(omega: Unit('rad / s'), kWave: Unit('rad / m'), T: Unit('K'), n: Unit('1 / m3'), particle, z_mean=None)[source]
Compute the classical dielectric permittivity for a 1D Maxwellian plasma.
This function can calculate both the ion and electron permittivities. No additional effects are considered (e.g. magnetic fields, relativistic effects, strongly coupled regime, etc.).
- Parameters:
omega (
Quantity
) – The frequency, in rad/s, of the electromagnetic wave propagating through the plasma.kWave (
Quantity
) – The corresponding wavenumber, in rad/m, of the electromagnetic wave propagating through the plasma.T (
Quantity
) – The plasma temperature — this can be either the electron or the ion temperature, but should be consistent with density and particle.n (
Quantity
) – The plasma density — this can be either the electron or the ion density, but should be consistent with temperature and particle.particle (
str
) – The plasma particle species.z_mean (
Real
) – The average ionization of the plasma. This is only required for calculating the ion permittivity.
- Returns:
chi – The ion or the electron dielectric permittivity of the plasma. This is a dimensionless quantity.
- Return type:
Notes
The dielectric permittivities for a Maxwellian plasma are described by the following equations (see p. 106 of Froula et al. [2011]):
\[ \begin{align}\begin{aligned}χ_e(k, ω) = - \frac{α_e^2}{2} Z'(x_e)\\χ_i(k, ω) = - \frac{α_i^2}{2}\frac{Z}{} Z'(x_i)\\α = \frac{ω_p}{k v_{Th}}\\x = \frac{ω}{k v_{Th}}\end{aligned}\end{align} \]\(χ_e\) and \(χ_i\) are the electron and ion permittivities, respectively. \(Z'\) is the derivative of the plasma dispersion function. \(α\) is the scattering parameter which delineates the difference between the collective and non-collective Thomson scattering regimes. \(x\) is the dimensionless phase velocity of the electromagnetic wave propagating through the plasma.
Examples
>>> import astropy.units as u >>> from numpy import pi >>> from plasmapy.formulary import thermal_speed >>> T = 30 * 11600 * u.K >>> n = 1e18 * u.cm**-3 >>> particle = 'Ne' >>> Z = 8 >>> vth = thermal_speed(T, particle, method="most_probable") >>> omega = 5.635e14 * 2 * pi * u.rad / u.s >>> k_wave = omega / vth >>> permittivity_1D_Maxwellian(omega, k_wave, T, n, particle, Z) <Quantity -6.72955...e-08+5.76163...e-07j>
For user convenience
permittivity_1D_Maxwellian_lite
is bound to this function and can be used as follows:>>> from plasmapy.formulary import plasma_frequency >>> wp = plasma_frequency(n, particle, Z=Z) >>> permittivity_1D_Maxwellian.lite( ... omega.value, k_wave.value, vth=vth.value, wp=wp.value ... ) (-6.72955...e-08+5.76163...e-07j)