Mathematical Difference Between Mean Free Path vs RMS Free Path?

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Discussion Overview

The discussion revolves around the mathematical differences between the RMS free path and the mean free path of molecules in an ideal gas. Participants explore the calculations involved in determining these paths, the implications of using average versus RMS velocities, and the physical significance of these concepts.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants question whether the RMS free path and mean free path yield different results, noting that their calculations seem to lead to the same value.
  • One participant emphasizes that the root mean square speed is an approximation of the mean speed, particularly in equilibrium conditions, and clarifies that mean speed is not the same as mean velocity.
  • Another participant argues that the mean square of the velocity relates to kinetic energy and temperature, suggesting that this connection is significant beyond mere approximation.
  • Some participants assert that the mean speed is more accurate than the RMS speed in determining the mean free path, though they do not clarify in what way it is more accurate.
  • There is a discussion about the physical significance of the RMS free path, with one participant questioning its relevance compared to other quantities like collision frequency and temperature.
  • Participants express uncertainty about how to measure mean time and mean speed, raising questions about the validity of using these measurements to calculate mean path.
  • A historical reference is made to Clausius's interpretation of mean free path, involving the concept of scattering cross-section and mean time between collisions.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the relationship between mean speed and RMS speed, as well as the significance of the RMS free path. The discussion remains unresolved, with no consensus on the superiority of one approach over the other.

Contextual Notes

Some participants highlight the dependence of their arguments on specific assumptions about the gas behavior and statistical distributions of speeds and times, which remain unresolved in the discussion.

RagincajunLA
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I was wondering if there is a mathematical difference between the RMS free path and the mean free path of molecules in an ideal gas. For example, When I calculate the mean free path, I use use the average velocity and the scattering rate which is a function of the average velocity. I then multiply the two and the average velocities cancel to produce the mean free path.

When I go to calculate the RMS free path, I assume I use the RMS velocity and the RMS scattering rate which is based on the RMS velocity. When I multiply these two, the RMS velocity cancels and I am left with the value as the mean free path. Is this correct? I assumed they would be different. My equations are...

A = \bar{v}\tau
\tau = \frac{1}{\sqrt{2}n \pi d^{2} \bar{v} }

A_{rms} = v_{rms}\tau_{rms}
\tau_{rms} = \frac{1}{\sqrt{2}n \pi d^{2} v_{rms} }​
 
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RagincajunLA said:
I was wondering if there is a mathematical difference between the RMS free path and the mean free path of molecules in an ideal gas. For example, When I calculate the mean free path, I use use the average velocity and the scattering rate which is a function of the average velocity. I then multiply the two and the average velocities cancel to produce the mean free path.

When I go to calculate the RMS free path, I assume I use the RMS velocity and the RMS scattering rate which is based on the RMS velocity. When I multiply these two, the RMS velocity cancels and I am left with the value as the mean free path. Is this correct? I assumed they would be different. My equations are...

A = \bar{v}\tau
\tau = \frac{1}{\sqrt{2}n \pi d^{2} \bar{v} }

A_{rms} = v_{rms}\tau_{rms}
\tau_{rms} = \frac{1}{\sqrt{2}n \pi d^{2} v_{rms} }​

If the bulk of the gas isn't moving then the average velocity is Zero, surely.
 
I think the root mean square speed is just an approximation to the mean speed. In equilibrium condition, it is a good approximation.
Mean speed is not mean velocity. In equilibrium mean velocity is zero.
 
It's a lot more than that. The mean square of the velocity is the mean kinetic energy of a set of particles with the same Mass. That corresponds to temperature, which is far more significant than just an 'approximation'.
The RMS Voltage in an AC circuit is the value of the DC equivalent voltage that would supply the same Power to a resistor.
RMS is a very useful quantity to get your head around. (The Standard Deviation of a statistical distribution is an excellent measure of the statistical 'spread' of a set of values.)
 
Arguable, in the determination of mean free path. it is the mean speed that is more accurate rather than the root mean square speed. The mean speed is quite different from the root mean square speed.
 
TSC said:
Arguable, in the determination of mean free path. it is the mean speed that is more accurate rather than the root mean square speed. The mean speed is quite different from the root mean square speed.

? more accurate?. In what way? Do you mean easier to measure accurately?
If you knew the statistics of the speed distribution (and you would have to, in any case) then you could deduce one from the other, in any case, depending upon which you were able to measure.

But i agree that, to know the time between collisions, it is the mean speed that counts. Does the speed influence the spacing, though? Surely, that is a function of the number of particles per unit volume.
 
Since we agree on that, I have to add, it is the mean relative speed.
 
I think of it as if a distribution is Gaussian or Poisson... then which one is better to use? and in what sense does accurate now means? just saying
 
  • #10
To return to the OP, I wonder what physical significance the RMS free path has. Apart from the fact that it may be 'possible to calculate', it strikes me as not having any particular meaning at all.
There are much quantities that would be of much more interest:
For instance, the frequency of collisions would be related to temperature (RMS speed) and MFP. Now, that has some physical significance. And the RMS speed, as mentioned before, would relate to temperature (always a relevant quantity)..
 
  • #11
Mean free path = mean speed * mean time.
This sounds so intuitive physically, that is why mean speed is more meaningful.
Note that mean free path is going to affect your viscosity, which has to be decided by experiment.
If you use rms speed, you may not agree with experiment.
 
  • #12
TSC said:
Mean free path = mean speed * mean time.
This sounds so intuitive physically, that is why mean speed is more meaningful.
Note that mean free path is going to affect your viscosity, which has to be decided by experiment.
If you use rms speed, you may not agree with experiment.

What I don't understand about this is how you intend to measure 'mean time'. You seem to be confusing a dependent variable with an independent variable. What experiments will give you mean time and mean speed, to let you calculate mean path?
Aamof, I even wonder whether the statistical distributions of time and speed lead to the valid use of your equation.
 
  • #13
This is done by Clausius in 1858.
Imagine you are a molecule with a smiling face waiting for other molecules to hit. The area of your face is call the scattering cross section. Imagine all these molecules move toward you with a mean speed, and with the number density, and the fact that all these molecules lie within a certain length of tube with a cross sectional area equals to the scattering cross section, you can calculate the mean time = time between molecules hitting your face.
This is how I interpret Clausius's mean free path.
 

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