Normalization

The characteristics of Langmuir probes do not depend on every conceivable parameter such as density, temperature, probe length, etc. independently, but instead upon a smaller set of non-dimensional groups (\pi-groups) of such parameters [Laframboise], [Marholm]. One such group is the normalized voltage:

\eta = -\frac{qV}{kT}

where q and T are the charge and temperature of the collected species, V is the voltage, and k is Boltzmann’s constant (for \eta>0 the species is attracted, and for \eta<0 it is repelled). It may therefore be of interest to study an entire class of problems with the same normalized parameters instead of a specific case. In Langmuir one may specify normalized voltages by using the argument eta instead of V in models such as OML_current.

Similarly, a normalized current I/I_0 may be defined, where I is the collected current and I_0 is a characteristic current. The models in Langmuir may return currents normalized by one of several possible characteristic currents depending on the value of the normalization argument:

  • 'th': Normalized by the thermal current. Often the most natural choice.
  • 'oml': Normalized by the current according to the OML theory. This is useful for comparing other models with OML theory.
  • 'thmax': Normalized by the thermal current of a Maxwellian plasma regardless of what the distribution actually is. This is the normalization used in [Darian].

Finally, all lengths are normalized by the Debye length \lambda_D. Below is a complete example of obtaining the normalized current for a cylindrical probe of radius 0.2\lambda_D and length 10\lambda_D with \eta=10:

>>> sp = Species()
>>> geometry = Cylinder(r=0.2*sp.debye, l=10*sp.debye)
>>> OML_current(geometry, sp, eta=10, normalization='th')
3.7388259506315147

Since only the non-dimensional groups determine the normalized collected current, we do not care about the exact parameters of the species, but leave them at the default. Note that in this case it actually does not matter what the probe size is, because the thermal current depends on the probe size in the same way as the current predicted by OML theory. This may differ for other models, however.

Note that the non-dimensional groups are specific to each species, e.g., the voltage normalized with respect to electrons is not the same as with respect to ions. If a multi-species plasma is specified, the normalization used will be with respect to the first species in the list. E.g., if electrons are the first element in the list, \eta=eV/kT_e where e is the elementary charge and T_e is the electron temperature.