Understanding the Debye Length in Plasma Physics

AI Thread Summary
The Debye length, denoted as λD, is the distance over which mobile charge carriers in a plasma can screen out an external electric field, effectively decaying the potential by a factor of 1/e. In plasma physics, L represents a characteristic length, often related to the mean distance between particle collisions, and is typically much larger than λD (L >> λD). This condition is crucial for distinguishing a plasma from a common ionized gas, alongside other criteria such as the number of charged particles and the frequency of plasma oscillation. The exponential decay of electric potential due to screening is a key concept in understanding plasma behavior. Resources like Richard Fitzpatrick's free book provide further insights into these principles.
Nylex
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Can someone explain to me what this is? All we were told in my Physics of Stars module was that for a plasma,

L \gg \lambda_{D}, where \lambda_{D} is the Debye length.

We were also told that it's an "e-folding distance" for a potential, but that doesn't help to understand it.

I'm not even sure what L is either (the length of the plasma?? :confused: ) :/.

Thanks.
 
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Nylex said:
Can someone explain to me what this is? All we were told in my Physics of Stars module was that for a plasma,

L \gg \lambda_{D}, where \lambda_{D} is the Debye length.

I'm not even sure what L is either - the length of the plasma??
In the context of a plasma, L is probably a characteristic length, as in the mean distance between successive particle collisions, for example.

In nuclear interaction, L = \frac {1}{\Sigma}, where \Sigma is the macroscopic cross-section of the particle interaction.

I assume the module is indicating that the distance between successive collisions of particles is much greater than the Debye length.
 
When you apply a potential diference to a plasma, electrons and ions will be attracted by the positive and negative electrodes respectively. The electric potential generated by the electrodes will then we screened out by the charged particles.The screening decays exponentially as you go away from the elctrode.
A debye length is the length by which the potential has decayed 1/e.-thats what they mean by an e-folding.
Big L in plasma means the characteristic length of the ''plasma''. Thats is, is you talk about space plasma, L is in the AU order, in tokamaks L is in the order of meters, in neon lamps L is in he order of centimeters...and so on.
The condition L>>ld is one of the 3 criteria that separates a common ionized gas from a plasma. The other 2 criteria are:
Nd>>1
wt>1
Where Nd is THE plasma parameter (number of charged particles in a spherical volume of radius ld), w is the frequency of typical plasma oscilation, and t is themean time between collisions.

I hope i was clear enough.=D
 
Previous posts are good. Another resource is the free book from Richard Fitzpatrick:

http://farside.ph.utexas.edu/teaching/plasma/380.pdf

see section 1.6. This is a very nice book. HIs derivation uses teh fact that for the vast majority of plasmas ("weakly coupled" - see section 1.7), classical statistics apply, and furthermore e \phi << k T.

I'm guessing your prof. means that the length scales you care about are much larger than a Debye length. This statement holds for hte vast majority of plasma physics.

jason
 
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Thanks for the pdf.
Looks promising =D
 
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