GREPhysics.NET
GR | # Login | Register
   
  GR9277 #72
Problem
GREPhysics.NET Official Solution    Alternate Solutions
\prob{72}
A system in thermal equilibrium at temperature T consists of a large number $N_0$ of subsystems, each of which can exist only in two states of energy $E_1$ and $E_2$, where $E_2-E_1=\epsilon \gt 0$. In the expressions that follow, k is the Boltzmann constant.

The internal energy of the system at any temperature T is given by $E_1N_0+\frac{N_0\epsilon}{1+e^{\epsilon/kT}}$. The heat capacity of the system is given by which of the following expressions?


  1. $N_0k \left(\frac{\epsilon}{kT}\right)^2\frac{e^{\epsilon/kT}}{\left(1+e^{\epsilon/kT}\right)^2}$
  2. $N_0k \left(\frac{\epsilon}{kT}\right)^2\frac{1}{\left(1+e^{\epsilon/kT}\right)^2}$
  3. $N_0k\left(\epsilon/kT\right)^2e^{-\epsilon/kT}$
  4. $N_0k\left(\epsilon/kT\right)^2$
  5. $3N_0k/2$

Statistical Mechanics}Heat Capacity

The heat capacity is just dU/dT, where ETS generously supplies U, the internal energy. Since E_1 and N_0 are constants, the first term is trivial.

The temperature-derivative of the second term is N_0\epsilon^2/(kT^2)e^{\epsilon/kT} /(1+e^{\epsilon/kT})^2=, as in choice (A).

(The temperature derivative is easily done if one applies the chain-rule \frac{df}{dy}\frac{dy}{du}\frac{du}{dT} where f=1/y, y=1+e^u, u=\epsilon/(kT).)

See below for user comments and alternate solutions! See below for user comments and alternate solutions!
Alternate Solutions
jmason86
2009-09-03 19:19:22
I did this one by limits and general test taking strategy.

Limits: Q --> finite value as T --> \infty. Eliminates (D) and (E)

ETS will generally force you to choose between very similar answers. Eliminates (C)

With only (A) and (B) left, it is a good idea to guess. But if you can get a hunch, that is even better. It's probably totally flawed thinking, but I saw the lack of an exponential in the numerator for (B), which made it look similar to a Bose-Einstein distribution. The full expression in (A) reminded me of the Maxwell-Boltzmann distribution that comes from the problem statement. Choose (A)
Alternate Solution - Unverified
Comments
ernest21
2019-09-30 05:00:43
Cool! I\'ll surely be coming back for the next posts from you. You\'re an incredibly engaging writer that I can freely recommend this article to my college students. clash royale best decksNEC
BerkeleyEric
2010-09-17 17:04:59
If you remember that C=\frac{dU}{dT}, then immediately you can see that there will have to be the squared sum in the denominator, so only A and B remain. And there still has to be the exponential in the numerator (a derivative won't get rid of that), so the answer must be A.
flyboy621
2010-10-22 16:11:48
+1
NEC
jmason86
2009-09-03 19:19:22
I did this one by limits and general test taking strategy.

Limits: Q --> finite value as T --> \infty. Eliminates (D) and (E)

ETS will generally force you to choose between very similar answers. Eliminates (C)

With only (A) and (B) left, it is a good idea to guess. But if you can get a hunch, that is even better. It's probably totally flawed thinking, but I saw the lack of an exponential in the numerator for (B), which made it look similar to a Bose-Einstein distribution. The full expression in (A) reminded me of the Maxwell-Boltzmann distribution that comes from the problem statement. Choose (A)
Alternate Solution - Unverified
RebeccaJK42
2007-03-23 10:27:19
Where does the k in the numerator come from?
alpha
2007-03-30 22:37:37
k is Boltzmann constant.. The k on the numerator is actually canceled out by the k^2 in the denominator
Richard
2007-09-14 00:05:03
The fact of the matter is, you have a factor of
\epsilon/k introduced by the derivative.
To make it look pretty, they multiplied the top and bottom by k giving (with the extra \epsilon) the factor k(\frac{\epsilon}{k})^2. Then of course, you have the T^2.
Answered Question!
Andresito
2006-03-29 10:05:29
I could not obtain T^2 in the denominator. Is there an error in the solution provided by the ETS?
radicaltyro
2006-10-31 14:19:25
Hi Andresito,

Review your calculus and try again. The answer is correct.
Blue Quark
2007-11-01 08:00:11
Andresito you made the same mistake I did. The T is in the denominator, not the numerator. Thus when you differentiate you get a (-T^(-2)) in front of the exponential in addition to the normal e/k
drizzo01
2012-11-08 07:40:44
am I the only one who doesn't see a T in the denominator of the second term? I appreciate that T^2 would be in the denominator if there was a T to being with, but as far as I can see, the only T's are within the expression for the exponential, which don't come out upon taking a derivative.
drizzo01
2012-11-08 07:46:58
wait nvm, got it.
Answered Question!

Post A Comment!
You are replying to:
If you remember that C=\frac{dU}{dT}, then immediately you can see that there will have to be the squared sum in the denominator, so only A and B remain. And there still has to be the exponential in the numerator (a derivative won't get rid of that), so the answer must be A.

Username:
Password:
Click here to register.
This comment is best classified as a: (mouseover)
 
Mouseover the respective type above for an explanation of each type.

Bare Basic LaTeX Rosetta Stone

LaTeX syntax supported through dollar sign wrappers $, ex., $\alpha^2_0$ produces .
type this... to get...
$\int_0^\infty$
$\partial$
$\Rightarrow$
$\ddot{x},\dot{x}$
$\sqrt{z}$
$\langle my \rangle$
$\left( abacadabra \right)_{me}$
$\vec{E}$
$\frac{a}{b}$
 
The Sidebar Chatbox...
Scroll to see it, or resize your browser to ignore it...