Kinetic Theory of Gases Average question

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SUMMARY

The discussion revolves around the Kinetic Theory of Gases, specifically the calculation of the root mean square velocity (\overline{v}) and its significance in understanding gas behavior. The user initially struggles with the mathematical concept of \overline{v}^2 = (1/n) ∑(v_i^2) and its application in deriving the total change in momentum as [2mn\overline{v}^2]/l. The conversation clarifies that the root mean square velocity represents the average speed of gas molecules, directly correlating to their kinetic energy and, consequently, the temperature of the gas. The user ultimately gains clarity on the concept, recognizing its importance in the context of gas dynamics.

PREREQUISITES
  • Understanding of basic physics concepts, particularly momentum and kinetic energy.
  • Familiarity with mathematical concepts such as summation and averages.
  • Knowledge of the Kinetic Theory of Gases and its implications in thermodynamics.
  • Basic grasp of statistical mechanics, particularly the concept of root mean square velocity.
NEXT STEPS
  • Study the derivation of the Kinetic Theory of Gases equations, focusing on momentum and energy relationships.
  • Learn about statistical mechanics and its application in thermodynamics.
  • Explore the concept of root mean square velocity in greater detail, including its derivation and significance.
  • Investigate the relationship between temperature and kinetic energy in gases, including practical examples.
USEFUL FOR

Students and professionals in physics and chemistry, particularly those studying thermodynamics, gas dynamics, or statistical mechanics. This discussion is beneficial for anyone seeking to deepen their understanding of molecular behavior in gases and the mathematical principles underlying these concepts.

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Hey I'm studying the Kinetic Theory of gases and although it's in a chemistry
book it employs physics concepts ergo I have come here to ask you nice people :biggrin:

The 5th point is where I have a problem, the rest is just information for you.

I am assuming a particle is in a cube (ideal situations here) & it traverses a
distance l with a momentum p=mv.

1. As it travels forward it will hit the cube wall and the resultant change in
momentum will be;
change \ in \ momentum \ = \ (mv) \ - \ (-mv) \ = \ 2mv

2. The number of collisions per second will be;
No.\ of \ collisions \ per \ second \ = \ \frac{velocity}{distance} \ = \ \frac{v}{l}

3. The Change in momentum per second will be;
Change \ in \ momentum \ per \ second = 2mv \frac{v}{l} \ = \ \frac{2mv^2}{l}

4. I've assumed one particle in one direction. Assuming n particles with
a total change in momentum per second of;
total \ change \ in \ momentum \ per \ second \ = \ \frac{2m}{l} \ \displaystyle\sum_{i=1}^n v_i^2

5. Here is where I have the problem. The text says to do this next;

Define the root square mean velocity, \overline{v} such that;
\overline{v}^2 \ = \ \left( \ \frac{1}{n} \ \sum_{i=1}^n v_i^2 \right)

What does this mean? Is this some mathematical concept from probabilities? I haven't done probabilities in math in like 5 years & even then that was in school . Where did the [(2m)/l] fraction go?

Using this concept the book goes on to show that;
The \ total \ change \ in \ momentum \ = \ [2mn \overline{v}^2 ] / l

(that is a fraction with l in the denominator, all the rest in the numerator [latex issues] )
I can't understand this (or any of the further concepts on pressure etc...) without getting this concept.
 
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The root mean square velocity is useful because it is the speed of a molecule that has an energy equal to the average energy of all the molecules in the gas. This is because the kinetic energy of a molecule is mv^2/2. If you add up all the squares of all the velocities of the molecules. multiply by m/2 and divide by n, you will get the average energy of the gas molecules. This is useful because the temperature of the gas is directly related (proportional to) the average energy of the gas molecules.

AM
 
I don't see any logic nor reason for doing that mathematically.

I understand that you are converting to using kinetic energy but I mean, it seems as though you're just arbitrarily multiplying one side by m/2 then dividing by n.

What about multiplying both sides of the equation?
Or multiplying top and bottom by a clever choice of 1?

http://www.betz.lu/media/users/charel/math07.gif
 
Last edited by a moderator:
2mv^2/l gives the force for just a single molecule of velocity v.If there are n such molecules all moving with the same velocity the total force would be n*2mv^2/l.The chance of the molecules all moving with the same velocity is very remote so instead of using v we use v bar(the mean squared velocity)which leads to the final equation you wrote.The 2m/l fraction hasn't gone anywhere.
 
OH!

God it's so easy lol...

I must be so tired that it's obviously affecting my study @ this stage.

So the average velocity is just the sum of the velocities of all of the particles divided by the number of particles.

Great stuff, it makes even more sense conceptually to use this seeing as they won't all be hitting the walls at the same time. yes, thanks a lot. :)

------have to stop being scared away by sigma's :p-----
 

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