Does the Debye Length Change with Applied Potential Strength in a Plasma?

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SUMMARY

The Debye length, denoted as λ_D, is the effective distance over which electrostatic potential disturbances are screened in a plasma. Increasing the charge of a point particle does not alter the Debye length; rather, it results in a higher density of ions or electrons within the existing Debye length. The potential in a plasma decays according to the formula φ_0 e^{-\frac{|x|}{λ_D}}, where φ_0 represents the applied potential. This decay rate remains constant regardless of whether a 1V or 10V potential is applied, indicating that the Debye length is independent of the strength of the applied potential.

PREREQUISITES
  • Understanding of plasma physics concepts
  • Familiarity with electrostatic potential and its behavior in plasmas
  • Knowledge of the Debye shielding effect
  • Basic mathematical skills to interpret exponential decay functions
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  • Study the mathematical derivation of the Debye length in plasmas
  • Explore the implications of Debye shielding on plasma stability
  • Investigate the effects of varying particle charge on plasma behavior
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Physicists, plasma researchers, and students studying plasma dynamics and electrostatics will benefit from this discussion, particularly those interested in the behavior of charged particles in plasma environments.

Sharkey4123
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The debye length is the effective length over which electrostatic potential disturbances are "screened out" in a plasma.

So if I drop a charged point particle in a plasma, then I expect after some Debye Length, D, from this point charge, I can see no difference between any other point in the plasma.

Now, if I were to increase the charge of that particle and drop it in the plasma again, would the Debye length still be the same as before? Even if I considered this new charged particle to have any arbitrarily large charge?

Surely, the electrostatic potential created by this new charge would be much larger than the previous case, and thus "extend" further, taking "more" of the plasma to screen it out, hence a larger Debye Length. Is this correct?
 
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I've probably figured this out myself, but should this be of use to anyone I'll leave it here for reference, or someone can correct me.

I believe that if I were to add a larger charge, there would simply be more ions/electrons (depending on the sign of the charge) attracted to within the Debye length.

So instead of an "increased" Debye length, I'd have more of the appropriate particle within the Debye length.
 
Roughly speaking if you apply a potential to a plasma then the potential in a plasma will decay as \phi_0 e^{-\frac{\left|x\right|}{\lambda_D}} where \lambda_D is the Debye length and \phi_0 is the applied potential.

The Debye length is a measure of how fast the applied potential decays. It is independent of the strength of the applied potential. It is the same if I apply a 1V potential or a 10V potential. However a larger potential will penetrate farther into a plasma. This isn't due to a change in the Debye length. You're just applying a stronger field so it takes more Debye lengths for it to decay away.
 

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