Highly collisional yet low resistivity plasmas

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Discussion Overview

The discussion revolves around the relationship between collisionality and resistivity in plasmas, particularly in the context of ideal magnetohydrodynamics (MHD). Participants explore how high collisionality can coexist with low resistivity, questioning the assumptions underlying these concepts in both theoretical and practical scenarios.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants question how high collisionality can lead to low resistivity, given that resistivity is often associated with collisions in the plasma.
  • Others propose that the resistivity may depend on the number of free electrons, suggesting that frequent collisions could create multiple parallel paths for current flow.
  • A participant discusses the calculation of energy loss in collisions, indicating that the energy loss rate is related to the momentum loss rate, particularly in electron-electron collisions.
  • Concerns are raised about the kinetic energy acquired from the overall field in dense plasmas being minimal, which could affect the energy loss during collisions.
  • Some participants express uncertainty about the resistivity in extreme conditions, questioning whether the interactions could be characterized as high impedance phenomena.
  • There is a suggestion that if collisions occur, they may not result in significant energy loss, leading to further inquiry into the conditions under which this might hold true.
  • A participant emphasizes the need to consider both macroscopic and microscopic models to understand the energy dynamics in collisional plasmas.

Areas of Agreement / Disagreement

Participants do not reach a consensus; multiple competing views remain regarding the relationship between collisionality and resistivity, and the discussion remains unresolved.

Contextual Notes

Limitations include assumptions about the nature of collisions, the definitions of resistivity and impedance in different plasma conditions, and the dependence on specific parameters like mean free path and kinetic energy.

TheCanadian
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In approximations for the applicability of ideal MHD to plasmas, it states that plasmas are considered highly collisional to permit the assumption that the plasma (i.e. electrons) follow a Maxwellian velocity distribution. Although is not resistivity based on collisions in the plasma? If there is high collisionality, how can this result in collisions that somehow have low resistivity?
 
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I would expect the resistivity to depend on the number of free electrons as much as anything. Frequent collisions would ensure that there were plenty of parallel paths for the current can take. But would the collisions necessarily transfer much net energy to thermal once equilibrium was established?
 
sophiecentaur said:
I would expect the resistivity to depend on the number of free electrons as much as anything. Frequent collisions would ensure that there were plenty of parallel paths for the current can take. But would the collisions necessarily transfer much net energy to thermal once equilibrium was established?

The number density of free electrons is certainly important in determining the rate of collisions. When considering momentum loss in plasmas, the rate is given in the first attachment. The actual magnitude for the energy loss would be calculated by multiplying the loss rate by the initial kinetic energy. Now if considering any collision in general (i.e. momentum loss rate), the ratio between the energy loss rate and momentum loss rate is given by the second attachment for thermal plasmas. If we're considering electron-electron collision to dominate (i.e. ##m_1 = m_2 = m_e##), then the two rates are equivalent. Thus in ideal MHD, why is it permissible to consider these plasmas to be highly collisional yet of low resistively if energy exchange does occur between individual particles during collisions?
 

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TheCanadian said:
The actual magnitude for the energy loss would be calculated by multiplying the loss rate by the initial kinetic energy.
In a dense plasma, the KE, acquired from the overall field would be tiny? (I'm trying to look for reasons why the loss would be much less than you suggest.)
 
I have no idea about such extreme conditions but what would be the Resistivity that you refer to above? Wouldn't it all be a pretty High Impedance phenomenon? Out perhaps the interactions wouldn't be losing much energy from the electrons - so not actual 'collisions'?
 
sophiecentaur said:
I have no idea about such extreme conditions but what would be the Resistivity that you refer to above? Wouldn't it all be a pretty High Impedance phenomenon? Out perhaps the interactions wouldn't be losing much energy from the electrons - so not actual 'collisions'?

For the impedance to be negligible in MHD, we're considering the case: ## \eta \bf\vec{J} \ll \bf\vec{E} + \bf\vec{v} \times \bf\vec{B} ##, where ##\eta## is resistivity. Well that's what I'm trying to understand (and try to demonstrate in the above attachments): if collisions do take place, why would the collisions result in negligible energy loss?
 
TheCanadian said:
For the impedance to be negligible in MHD, we're considering the case: ## \eta \bf\vec{J} \ll \bf\vec{E} + \bf\vec{v} \times \bf\vec{B} ##, where ##\eta## is resistivity. Well that's what I'm trying to understand (and try to demonstrate in the above attachments): if collisions do take place, why would the collisions result in negligible energy loss?

If the mean free path is low and the field is low then how much KE can be gained before a collision. If you can find those two values then you can find the velocity gained and hence the KE lost per interaction. Your equation is macroscopic whilst you need the microscopic model to give you the number you want.
 

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