Maxwell Boltzmann Distribution Question

AI Thread Summary
The discussion revolves around determining the constant C in the Maxwell-Boltzmann distribution for a two-dimensional gas, ensuring that the integral of the distribution equals N. The user attempts to integrate the function but struggles with evaluating the integral at infinity. Guidance is provided to evaluate the integral from 0 to a variable t, then take the limit as t approaches infinity. The user finds that the limit leads to an expression involving C, k, and T, but seeks confirmation on whether they have missed any critical steps in the process. The conversation emphasizes the importance of correctly evaluating the integral to solve for C.
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Hello everyone

Homework Statement


The equivalent of the Maxwell-Boltzman distribution for a two-dimensional
gas is
P(v) = Cv e^-\frac {mv^2}{kt}

Determine C so that

\int_0^\infty P(v)dv = N

Homework Equations


Not really sure

The Attempt at a Solution


I wasn't really sure how to tackle this question so I figured i'd integrate P(v) since the question says that'll equal N.

\int_0^\infty P(v)dv
\int_0^\infty Cv e^-\frac {mv^2}{kt} dv
C\int_0^\infty v e^-\frac {mv^2}{kt} dv

u = \frac {mv^2}{kt}

\frac {du}{dv} = \frac {2mv}{kt}

dv = \frac {du kt}{2mv}

C\int_0^\infty v e^{-u} \frac {du kt}{2mv}

C\int_0^\infty e^{-u} \frac {du kt}{2m}

\frac {Ckt}{2m} \int_0^\infty e^{-u} du

= \frac {Ckt}{2m} \bigg[{-e^{-u}\bigg]_0^\infty

= \frac {Ckt}{2m} \bigg[{-e^{-\frac {mv^2}{kt}}\bigg]_0^\infty

I'm not really sure where to go from here. How would I evaluate this between infinity and zero?

Thanks
 
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HINT: You said the entire integral has to equal N, correct? Well, your last line is equal to the integral. So if A = B and B=C ... ?
 
ok, so you're saying

N = \frac {Ckt}{2m} \bigg[{-e^{-\frac {mv^2}{kt}}\bigg]_0^\infty

which yeah, makes sense. But do you want me to rearrange it to make C the subject while not evaluating the integral?
 
Crosshash said:
ok, so you're saying

N = \frac {Ckt}{2m} \bigg[{-e^{-\frac {mv^2}{kt}}\bigg]_0^\infty

which yeah, makes sense. But do you want me to rearrange it to make C the subject while not evaluating the integral?

No. Evaluate the integral and then solve for C. That should be your answer.
 
G01 said:
No. Evaluate the integral and then solve for C. That should be your answer.

I thought so. This might seem stupid, but I really don't know how to evaluate the integral when one of the limits is \infty. Could you shed some light on that please?
 
Crosshash said:
I thought so. This might seem stupid, but I really don't know how to evaluate the integral when one of the limits is \infty. Could you shed some light on that please?

To evaluate your integral, evaluate the following instead:

N = \frac {Ckt}{2m} \bigg[{-e^{-\frac {mv^2}{kt}}\bigg]_0^t

Now take that whole resulting expression and take the limit as t\rightarrow\infty.

Now can you solve for C?
 
G01 said:
To evaluate your integral, evaluate the following instead:

N = \frac {Ckt}{2m} \bigg[{-e^{-\frac {mv^2}{kt}}\bigg]_0^t

Now take that whole resulting expression and take the limit as t\rightarrow\infty.

Now can you solve for C?

Ok, so \bigg[{-e^{-\frac {mv^2}{kT}}\bigg]_0^t

will give me

\lim_{t \to \infty}({-e^{-\frac {mt^2}{kT}} + 1)

yeah?

Sorry if this is annoying, I've never actually done something like this which seems a bit strange considering a question requires it. I appreciate the help.
 
I used a site that provides a nice integral and limit calculator:
http://www.numberempire.com/limitcalculator.php
From that, I get:

\[\lim_{v\to0}\left(-{{k\,T\,e^ {- {{m\,v^2}\over{k\,T}} }}\over{2\,m}}\right) = -{{k\,T}\over{2\,m}}\]
So:
\[C \times \left[ \frac{kTe^{\frac{-mv^2}{kT}}}{2m}\right]^{\infty}_0=C\times \frac{kT}{2m}\]

Have I missed something obvious?
 
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