Temperature negative thermodynamics

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SUMMARY

The discussion centers on the theoretical implications of negative temperatures in thermodynamics, specifically regarding the relationship between internal energy (U) and volume (V). It is established that negative temperatures can only be discussed in systems with a finite number of energy levels, as traditional systems with infinite levels do not accommodate negative energy. The Boltzmann factor is referenced to illustrate the behavior of particle distribution at negative temperatures, where the number of particles in higher energy states exceeds those in lower states. The challenge remains in determining how volume affects internal energy under these conditions.

PREREQUISITES
  • Understanding of thermodynamic concepts, particularly internal energy (U) and temperature (T).
  • Familiarity with the Boltzmann distribution and its implications in statistical mechanics.
  • Knowledge of finite versus infinite energy level systems in thermodynamics.
  • Basic principles of thermodynamic equations and their applications.
NEXT STEPS
  • Research the implications of negative temperatures in finite systems, focusing on specific examples.
  • Study the Boltzmann factor and its role in particle distribution at varying temperatures.
  • Explore the relationship between internal energy and volume in thermodynamic systems.
  • Investigate experimental setups that have demonstrated negative temperatures in controlled environments.
USEFUL FOR

Students of thermodynamics, physicists exploring statistical mechanics, and researchers interested in the properties of systems exhibiting negative temperatures.

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Homework Statement


Hi!
I have this question "how is the curve of U(internal energy) with volume if the temperature is negative"?

Homework Equations

The Attempt at a Solution


i cnsidered T=(partial U/partial S) at constant V and N (number of particules, but now i can't say the change of U with V if T<0...can somebody help me?
i also thought that T = slope of the tangent line to the function U(S) but i can't say how is the curve U(V) when T<0 as required

(note: i know the temperature can't be negative but we want to know what theoricaly happens)

thanks!
 
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Well, let's talk about Boltzmann factor a little bit. You know that the number of particles in an energy level is proportional to e^{-\frac{E_i}{kT}}, where E_i is the energy of that level. So If I compare the number of particles in two levels i and j where E_j&gt;E_i, I have \frac{N_j}{N_i}=\frac{ e^{-\frac{E_j}{kT}} }{ e^{-\frac{E_i}{kT}} }. But its obvious that for any finite positive temperature, N_j&lt;N_i and even when we have T\to \infty, its only that N_j=N_i. But let's just assume(as you did), that its possible to have T&lt;0. We then see that for negative temperatures, we have N_j&gt;N_i. But wait, there is something weird happening here. Of course when particles go to upper energy levels, it means they are getting energy from somewhere. But when the system has an infinite number of energy levels, as particles get more energy, they just keep moving up. So when we have infinite number of levels(as it is with the usual systems we think about), negative energy can't be accommodated into the theory and so if we want to think about negative temperatures, we should think about systems with finite number of levels. Its hard to explain but physicists actually found such systems(in fact not actually found them, but built them with some tricks) and achieved negative temperatures. So only in this restricted class of systems, we can talk about negative temperatures. But honestly I don't know how to get volume into play here. So I hope other people will contribute to this thread.
 

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