Thermal motion of an ionised gas molecule in an electric field

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Discussion Overview

The discussion focuses on the behavior of thermal velocity in ionised gas molecules when subjected to an electric field. Participants explore the implications of electric fields on the motion of charged particles, particularly in relation to their thermal velocities and the effects of collisions in a gas environment.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant proposes that the velocity gained by an ion due to a potential difference can be calculated using the equation eV = ½mv², questioning whether this velocity adds to the existing thermal velocity of the gas molecules.
  • Another participant notes that while charged particles are generally accelerated by electric fields, the situation for ionised molecules is complicated by collisions that randomise their velocity after traveling a mean-free-path.
  • A comparison is made to a column of gas in a gravitational field, suggesting that in thermal equilibrium, pressure differences do not imply temperature differences, but this analogy raises confusion for some participants regarding the role of thermal velocity.
  • One participant challenges the analogy, emphasizing that thermal velocity should not simply disappear when an ionised gas molecule is placed in an electric field.
  • Another participant references the Drude Model and statistical mechanics, indicating that the motion of conduction electrons is relevant to the discussion, but acknowledges differences between electrons and ionised molecules.
  • A participant argues that the mass of ionised molecules is significant compared to their thermal momentum, unlike conduction electrons, which are nearly massless.
  • There is a debate about the relevance of gravitational effects on gas molecules, with some asserting that gravity is negligible compared to the velocity of the molecules.
  • One participant emphasizes the importance of clearly stating the parameters of the question, particularly regarding the role of gravity in the context of the discussion.

Areas of Agreement / Disagreement

Participants express differing views on the impact of electric fields on thermal velocity, the relevance of gravitational effects, and the comparison between ionised molecules and conduction electrons. The discussion remains unresolved with multiple competing perspectives present.

Contextual Notes

Participants highlight the complexity of the interactions between thermal motion, electric fields, and collisions in gases, indicating that assumptions about the negligible effects of gravity may not hold in all contexts.

pranj5
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What I want to discuss here is what happens to the thermal velocity when an ionised gas molecule has been put into an electric field. Due to the charge (e) and potential difference (V), how much velocity has been gained by the ion can be calculated easily.eV = ½mv2

Where e is the charge of the ion, V is the potential difference, m is the mass of the ion and v is the velocity gained due to the potential difference.

From the formula above, it can be easily calculated that

v = https://www.physicsforums.com/file:///C:/Users/Payel/AppData/Local/Temp/msohtmlclip1/01/clip_image002.gif

Now, question is, the gas molecule already has its velocity due to the temperature of the gas that is the Root Mean Square velocity of molecules at that temperature. I want to know whether the velocity gained by the potential difference will be added to the velocity or not.
 
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In general, yes, a charged particle, whatever its velocity, will be accelerated by an electric field. But for an ionised molecule in a gas the situation is a bit more complicated, because after it has traveled one mean-free-path the ion is likely to collide with another molecule. At that point its velocity will be randomised. With gases at normal pressures, the potential difference corresponding to a physical distance of one mean-free-path may be quite low, and in those cases the field would produce a slight heating of the gas.
 
It's analogous to a column of gas in a gravitational field. In thermal equilibrium, the bottom isn't any hotter than the top; it's just at higher pressure.
On the other hand, if the density is very low, such that collisions are infrequent, then the particles at the bottom are moving faster than the particles at the top, but you would not have a Maxwell-Boltzmann distribution so the term thermal velocity would not be appropriate.
 
Khashishi said:
It's analogous to a column of gas in a gravitational field. In thermal equilibrium, the bottom isn't any hotter than the top; it's just at higher pressure.
How that can be I just simply can't understand.
Khashishi said:
On the other hand, if the density is very low, such that collisions are infrequent, then the particles at the bottom are moving faster than the particles at the top, but you would not have a Maxwell-Boltzmann distribution so the term thermal velocity would not be appropriate
Thermal velocity simply means that the random velocity of molecules of gases. When a gas molecule is ionised and put inside an electric field, how can the thermal velocity just disappear?
 
Please look up the Drude Model.

What you are asking is identical to the motion of conduction electrons in a standard, simple metal. You need to know a bit of statistical mechanics and the Boltzmann distribution. Unfortunately, your posts do not say much on whether this is something you already know, or capable of comprehending.

Zz.
 
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Being a student of physics, I know both. But ionised molecules are different from conduction electrons. Electrons are almost massless and their thermal momentum is negligible in comparison to motion due to electric field. That's not the case for an ion.
 
pranj5 said:
Being a student of physics, I know both. But ionised molecules are different from conduction electrons. Electrons are almost massless and their thermal momentum is negligible in comparison to motion due to electric field. That's not the case for an ion.

I looked again at your first post, and nowhere in there did you indicate that gravitational field plays a role. All you said was "...I want to discuss here is what happens to the thermal velocity when an ionised gas molecule has been put into an electric field..." Did I miss it?

It is imperative that you state clearly the parameters of your question. Both your first post and the title made no indication that you are also considering the weight of these ions. Otherwise, I feel like I'm chasing a moving target.

Zz.
 
When discussing gas laws, it has been considered that the weight of molecules is so small in comparison to their velocity that gravity plays actually very little or no part here. That's as far as I know.
 
pranj5 said:
When discussing gas laws, it has been considered that the weight of molecules is so small in comparison to their velocity that gravity plays actually very little or no part here. That's as far as I know.

So then, why is this any different than the conduction electrons if the weight is ignored? Do you want to care about the minuscule effect of gravity or not?

Zz.
 
  • #10
You haven't noticed that in case of electrons, I have used momentum, not mass.
 
  • #11
pranj5 said:
You haven't noticed that in case of electrons, I have used momentum, not mass.

How does this answer my question?

This is like pulling teeth.

Zz.
 
  • #12
Gas molecules have little mass but their velocity is high. That means we can neglect gravity as the mass is small but not the momentum as the velocity is sufficiently high.
 

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