How Can You Derive the Average Velocity in a Maxwell-Boltzmann Distribution?

  • Thread starter Thread starter AStaunton
  • Start date Start date
  • Tags Tags
    Maxwell
Click For Summary
SUMMARY

The discussion focuses on deriving the average velocity, v_average, in a Maxwell-Boltzmann distribution, specifically using the formula v_average = sqrt(8kT/(pi)m. The user outlines their integration process, starting from the probability density function f(v) = 4π(m/(2πmkT)^(3/2))v^2e^(-mv^2/(2kT)). They encounter discrepancies in their final result, particularly regarding the sign and the coefficients in the square root, ultimately realizing the error stemmed from misinterpreting the exponential term. The correct average velocity expression is confirmed to be sqrt(8kT/(mπ)).

PREREQUISITES
  • Understanding of Maxwell-Boltzmann distribution
  • Familiarity with integration techniques, particularly integration by parts
  • Knowledge of statistical mechanics concepts, including temperature (T), Boltzmann constant (k), and mass (m)
  • Proficiency in manipulating exponential functions and substitutions in calculus
NEXT STEPS
  • Study the derivation of the Maxwell-Boltzmann distribution in detail
  • Learn advanced integration techniques, specifically integration by parts and substitutions
  • Explore statistical mechanics principles related to kinetic theory
  • Investigate common errors in deriving physical equations from probability distributions
USEFUL FOR

Students and professionals in physics, particularly those focused on statistical mechanics and thermodynamics, as well as educators teaching these concepts.

AStaunton
Messages
100
Reaction score
1
maxwell Boltzmann (very sorry!)

I attempted to post this already but the latex code didn't work out and also the edit command didn't seem to work...so I am reposting, very sorry for the duplicate but do not know how to remove original!:

trying to show v_average=sqrt(8kT/(pi)m) using max boltz. distrib.:

f(v)=4\pi(\frac{m}{2\pi mkT})^{\frac{3}{2}}v{}^{2}e^{-\frac{mv^{2}}{2kT}}

to start with the formula is:

\langle v\rangle=\int_{0}^{\infty}vf(v)dv

to solve this need substitution x=v^2 and this gives dx=2vdv which gives 1/2dx=vdv and so leads to:

4\pi(\frac{m}{2\pi kT})^{\frac{3}{2}}\frac{1}{2}\int_{0}^{\infty}xe^{-mx/kT}dx

can now integrate the above by parts:

u=x dv=e^-mx/kT
du=dx v=-(kT/m)e^-mx/kT


the uv expression evaluates to 0 and so the final part of interest I am left with is:

\frac{kT}{m}\int_{0}^{\infty}e^{-mx/kT}dx=-\frac{k^{2}T^{2}}{m^{2}}e^{-mx/kT}|_{0}^{\infty}=-\frac{k^{2}T^{2}}{m^{2}}

not forgetting the constant term that was brought outside integral at very start:

(2\pi(\frac{m}{2\pi kT})^{\frac{3}{2}})(-\frac{k^{2}T^{2}}{m^{2}})=-\sqrt{\frac{kT}{2m\pi}}

this is my final answer and is in disagreement with the answer I should have gotten for two reasons:
the sign is clearly wrong and also instead of sqrt2 on the bottom I should have sqrt8 on the top:

\sqrt{\frac{8kT}{m\pi}}

Can anyone suggest where problem is, as I have rechecked a few times and I keep coming out with the same answer.
 
Physics news on Phys.org


OK, just figured saw why I got the sqrt2 on the bottom instead of sqrt8 on the top:
the expression has e^-mv^2/2kT I thought it was simply e^-mv^2/kT.

Still can't see where the sign went wrong though
 

Similar threads

  • · Replies 5 ·
Replies
5
Views
744
Replies
16
Views
2K
Replies
2
Views
2K
Replies
2
Views
1K
  • · Replies 3 ·
Replies
3
Views
662
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 16 ·
Replies
16
Views
1K
Replies
6
Views
3K
  • · Replies 17 ·
Replies
17
Views
2K