Debye length
In plasma physics, the Debye length, named after the Dutch physical chemist Peter Debye, is the scale over which mobile charge carriers (e.g. electrons) screen out electric fields in plasmas and other conductors. In other words, the Debye length is the distance over which significant charge separation can occur. A Debye sphere is a volume whose radius is the Debye length, in which there is a sphere of influence, and outside of which charges are screened.
In space plasmas where the electron density is relatively low, the Debye length may reach macroscopic values, such as in the Magnetosphere, Solar wind, Interstellar medium and Intergalactic medium (see table):
Plasma | Density n_{e}(m^{3}) | Electron temperature T(K) | Magnetic field B(T) | Debye length λ_{D}(m) |
Gas discharge | 10^{16} | 10^{4} | -- | 10^{−4} |
Tokamak | 10^{20} | 10^{8} | 10 | 10^{−4} |
Ionosphere | 10^{12} | 10^{3} | 10^{−5} | 10^{−3} |
Magnetosphere | 10^{7} | 10^{7} | 10^{−8} | 10^{2} |
Solar core | 10^{32} | 10^{7} | -- | 10^{−11} |
Solar wind | 10^{6} | 10^{5} | 10^{−9} | 10 |
Interstellar medium | 10^{5} | 10^{4} | 10^{−10} | 10 |
Intergalactic medium | 1 | 10^{6} | -- | 10^{5} |
http://www.pma.caltech.edu/Courses/ph136/yr2002/
Hannes Alfvén pointed out that: "In a low density plasma, localized space charge regions may build up large potential drops over distances of the order of some tens of the Debye lengths. Such regions have been called electric double layers. An electric double layer is the simplest space charge distribution that gives a potential drop in the layer and a vanishing electric field on each side of the layer. In the laboratory, double layers have been studied for half a century, but their importance in cosmic plasmas has not been generally recognized.".
Debye length in a plasma
In a plasma, the Debye length is
- [math] \lambda_D = \sqrt{\frac{\varepsilon_0 k/q_e^2}{n_e/T_e+\sum_{ij} j^2n_{ij}/T_i}}[/math]
where
- λ_{D} is the Debye length,
- ε_{0} is the permittivity of free space,
- k is Boltzmann's constant,
- q_{e} is the charge on an electron,
- T_{e} and T_{i} are the temperatures of the electrons and ions, respectively,
- n_{e} is the density of electrons,
- n_{ij}'is the density of atomic species i, with positive ionic charge jq_{e}
The ion term is often dropped, giving
- [math] \lambda_D = \sqrt{\frac{\varepsilon_0 k T_e}{n_e q_e^2}}[/math]
although this is only valid when the ions are much colder than the electrons.
Debye length in an electrolyte
In an electrolyte, the Debye length is
- [math] \lambda_D = \sqrt{\frac{\varepsilon_0 \varepsilon_r k T}{2 N_A e^2 I}}[/math]
where
- I is the ionic strength of the electrolyte,
- ε_{0} is the permittivity of free space,
- ε_{r} is the dielectric constant,
- k is the Boltzmann's constant,
- T is the Temperature,
- N_{A} is Avogadro's Number.
- e is the elementary charge,
or when the solute is mono-monovalent and symmetrical,
- [math] \lambda_D = \sqrt{\frac{\varepsilon_0 \varepsilon_r R T}{2 F^2 C_0}}[/math]
where
- R is the gas constant,
- F is the Faraday constant,
- C_{0} is the molar concentration of the electrolyte.