Calculating the Limit of an Einstein Solid Specific Heat

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SUMMARY

The limit of the specific heat of an Einstein solid as temperature approaches infinity is calculated using L'Hôpital's rule. The formula is given by lim_{T \to \infty} 3Nk {(\epsilon/kT)}^2 \frac{e^{(\epsilon/kT)}}{{(e^{(\epsilon/kT)}-1)}^2}, which simplifies to 3Nk after applying the rule twice. The change of variables y = \frac{\epsilon}{kT} is crucial, leading to the limit lim_{y \to 0} 3Nk\frac{y^2 e^y}{(e^y - 1)^2}. This calculation confirms that the specific heat approaches the Dulong-Petit limit at high temperatures.

PREREQUISITES
  • Understanding of L'Hôpital's rule in calculus
  • Familiarity with the concept of limits in mathematical analysis
  • Basic knowledge of thermodynamics and specific heat
  • Understanding of the Einstein solid model in statistical mechanics
NEXT STEPS
  • Study the application of L'Hôpital's rule in various limit problems
  • Explore the derivation of the specific heat of an Einstein solid
  • Learn about the Dulong-Petit law and its significance in thermodynamics
  • Investigate the relationship between temperature and specific heat in different materials
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Students and professionals in physics, particularly those focusing on thermodynamics and statistical mechanics, as well as anyone interested in advanced calculus applications.

Amok
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So, I can't really find this limit:

[tex]\lim_{T \to \infty} \ 3Nk {(\epsilon/kT)}^2 \frac{e^{(\epsilon/kT)}}{{(e^{(\epsilon/kT)}-1)}^2}[/tex]

This is actually the formula for the specific heat of an Einstein solid, which is pretty easy to derive but I haven't been able to calculate the limit to show it becomes Dulong-Petit at height temperatures. Maybe I've been missing something simple... I don't see how you could use l'Hopital's rule.

note: I wasn't sure whether I should post this in one of the physics forums, but I figured it's more of a calculus problem at this point.
 
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I think you can use L'Hôpital's rule. First of all, I made the change of variables
[tex] y = \frac{\epsilon}{kT}[/tex]
so that [itex]y \to 0[/itex] as [itex]T \to \infty[/itex]. This yields
[tex] \lim_{y \to 0} 3Nk\frac{y^2 e^y}{(e^y - 1)^2}[/tex]
which is of the form [itex]\frac{0}{0}[/itex]. Using L'Hôpital's rule, this equals
[tex] \lim_{y \to 0} 3Nk \frac{2y e^y + y^2 e^y}{2(e^y -1)e^y} = 3Nk \lim_{y \to 0} \frac{2y + y^2}{2e^y -2}[/tex]
which is once again of the form [itex]\frac{0}{0}[/itex]. Applying LH again, we get
[tex] 3Nk \lim_{y \to 0} \frac{2 + 2y}{2 e^y} = 3Nk \lim_{y \to 0} \frac{y +1}{e^y} = 3Nk \frac{0 +1}{1} = 3Nk[/tex]

I hope this helps: hopefully I didn't make any mistakes!
 
spamiam said:
I think you can use L'Hôpital's rule. First of all, I made the change of variables
[tex] y = \frac{\epsilon}{kT}[/tex]
so that [itex]y \to 0[/itex] as [itex]T \to \infty[/itex]. This yields
[tex] \lim_{y \to 0} 3Nk\frac{y^2 e^y}{(e^y - 1)^2}[/tex]
which is of the form [itex]\frac{0}{0}[/itex]. Using L'Hôpital's rule, this equals
[tex] \lim_{y \to 0} 3Nk \frac{2y e^y + y^2 e^y}{2(e^y -1)e^y} = 3Nk \lim_{y \to 0} \frac{2y + y^2}{2e^y -2}[/tex]
which is once again of the form [itex]\frac{0}{0}[/itex]. Applying LH again, we get
[tex] 3Nk \lim_{y \to 0} \frac{2 + 2y}{2 e^y} = 3Nk \lim_{y \to 0} \frac{y +1}{e^y} = 3Nk \frac{0 +1}{1} = 3Nk[/tex]

I hope this helps: hopefully I didn't make any mistakes!

That makes perfect sense. For some reason I forgot that there is also an inverse exponential in the numerator (I was thinking it was just an exponential). Thanks a bunch dude.
 

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