Debye length: Difference between revisions

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A plasma consisting of freely moving positively and negatively charged particles has a natural tendency to shield net charges (or cancel DC electric fields).
A plasma consisting of freely moving positively and negatively charged particles has a natural tendency to shield net charges (or cancel DC electric fields).
The effective shielding length is the Debye length, and can be derived from a simple two fluid model of the plasma.
The effective shielding length is the Debye length, and can be derived from a simple two fluid model of the plasma.
<ref>J.P. Freidberg, ''Plasma physics and fusion energy'', Cambridge University Press (2007) ISBN 0521851076</ref>
<ref>J.P. Freidberg, ''Plasma physics and fusion energy'', Cambridge University Press (2007) {{ISBN|0521851076}}</ref>
<ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref>
<ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) {{ISBN|3540242171}}</ref>


:<math>\lambda_D = \left ( \frac{\varepsilon_0 T_e}{e^2 n_0}\right )^{1/2}</math>
:<math>\lambda_D = \left ( \frac{\varepsilon_0 T_e}{e^2 n_0}\right )^{1/2}</math>

Latest revision as of 11:27, 26 January 2023

A plasma consisting of freely moving positively and negatively charged particles has a natural tendency to shield net charges (or cancel DC electric fields). The effective shielding length is the Debye length, and can be derived from a simple two fluid model of the plasma. [1] [2]

λD=(ε0Tee2n0)1/2

where Te is given in energy units.

See also

References

  1. ↑ J.P. Freidberg, Plasma physics and fusion energy, Cambridge University Press (2007) ISBN 0521851076
  2. ↑ K. Miyamoto, Plasma Physics and Controlled Nuclear Fusion, Springer-Verlag (2005) ISBN 3540242171