Why Does My Calculation of Maxwellian Gas Velocity Yield an Incorrect Result?

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Homework Help Overview

The discussion revolves around the calculation of Maxwellian gas velocities, specifically focusing on the root mean square (RMS) velocity and the average velocity of gas molecules. Participants are examining the relationships between these quantities and the implications of their definitions in the context of the Maxwell-Boltzmann distribution.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the calculation of RMS and average velocities, questioning the definitions and values assigned to these quantities. There is confusion regarding the interpretation of average velocity and its implications on the calculations presented.

Discussion Status

Some participants have provided insights into the definitions of average velocity and RMS velocity, while others are seeking clarification on the apparent contradictions in the calculations. The discussion is ongoing, with various interpretations being explored.

Contextual Notes

There is a noted assumption that the average velocity is zero, which is being questioned in light of the calculations involving squared terms. Participants are also considering the implications of working with vector quantities versus scalar magnitudes in their reasoning.

Saptarshi Sarkar
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Homework Statement
Calculate the value of ##<(v-\bar v)²>## for a Maxwellian gas
Relevant Equations
##<(v-\bar v)²> = <v²> + <\bar v²> - 2<v><\bar v>##
I expanded it as shown above and got

##<v²> + <\bar v²> - 2<v><\bar v>## = ##v_{rms}^2 + \bar v^2 = \frac {3kT} m+\frac {8kT} {πm}##

I used ##<v> = 0## as the velocity is equally likely to be positive as it's likely to be negetive.

From the above I get the answer ##\frac {kT} m(3+\frac 8 π)## but, the answer should be ##\frac {kT} m(3-\frac 8 π)##

Please help me understand what I did wrong.
 
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I don't understand either answer. What does ##\bar v## represent here? Isn't it the same as ##\langle v \rangle## so should be 0?
 
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vela said:
I don't understand either answer. What does ##\bar v## represent here? Isn't it the same as ##\langle v \rangle## so should be 0?

##\bar v## is the average velocity of the molecules in the gas and it is the same as ##<v>##, it would be 0 if the difference was not squared. The term ##<(v - \bar v)^2>## is the Variance of the velocity distribution.
 
So you're saying ##v_{\rm rms}^2 = \frac {3kT}{m} + \frac{8 k T}{\pi m}##? Can you explain how you got that?
 
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vela said:
So you're saying ##v_{\rm rms}^2 = \frac {3kT}{m} + \frac{8 k T}{\pi m}##? Can you explain how you got that?

##\frac {3kT}{m}## & ##\frac{8kT}{\pi m}## are respectively the formulas for the square of the RMS and Average velocities of a molecule in a gas according to Maxwell-Boltzmann distribution.
 
Saptarshi Sarkar said:
##\frac {3kT}{m}## & ##\frac{8kT}{\pi m}## are respectively the formulas for the square of the RMS and Average velocities of a molecule in a gas according to Maxwell-Boltzmann distribution.
How do you reconcile this statement with your earlier statement that the average velocity is 0?
 
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vela said:
How do you reconcile this statement with your earlier statement that the average velocity is 0?

I think I understood! ##v## cannot be negetive as it is velocity in 3D (##\vec v = v_x\hat i + v_y\hat j + v_z\hat k##) and it's magnitude must be positive! Only the average of ##v_x,v_y,v_z## would be 0.

Thanks a lot!
 
Saptarshi Sarkar said:
I think I understood! ##v## cannot be negative as it is velocity in 3D (##\vec v = v_x\hat i + v_y\hat j + v_z\hat k##) and its magnitude must be positive! Only the average of ##v_x,v_y,v_z## would be 0.
I think you're working with velocities, not speeds, in this problem. That is, ##v## and ##\bar v## both represent vectors, not the magnitudes. If this is the case, you generally have
$$\langle (v-\bar v)^2 \rangle = \langle (v-\bar v)\cdot (v-\bar v) \rangle = \langle v^2 \rangle - 2\langle v \cdot \bar v \rangle + \langle \bar v^2 \rangle.$$ You can show that
$$\langle v \cdot \bar v \rangle = \langle v \rangle \cdot \bar v = \bar v \cdot \bar v$$
 
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