hasan_researc said:
Thank you so much! Your answer's greatly helped me. I have just two more questions.
"I've skipped a lot of details here. What is thermal energy? It's a measure of the average energy of a system, given that it's at some temperature T":
Do you mean the average of the total internal energy (I mean excluding the energy due to ordered motion of the particles?
Yeah so internal energy is the total energy that arises due to random, or statistical events. I think I used the world "average" sloppily: The internal energy, U, is the total energy of the system of N particles, and if you divide the internal energy by the number of particles, U/n, that's now the average energy per particle (though whether or not U is an
exact or
average value I think depends on the kind of system you consider: in the microcanonical ensemble U is exact; in the canonical ensemble U is probabilistic...in any case, it's not a big deal for now). Among the things we
don't consider to be part of internal energy are: center of mass motion (e.g., a tank of water moving at speed v has the same internal energy as a stationary tank), relativistic energy (mc^2), gravitational potential energy, etc..
But then trnaslation and vibration are one and the only thing, isn't it?
No, translation is different from vibration (..is that what you're asking?..I'm not sure). You can have translational degrees of freedom without any vibrations. E.g. a 3D free, non-interacting gas has 3 degrees of freedom, while a 3D crystal lattice (where you model the atom-atom bonds as springs) as 6 degrees of freedom.
The slightly longer story to the equipartition theorem is that if you write out the total energy for your particle(s) in question, then for each quadratic term you get 0.5kT of energy. For example, the total energy of a single moving particle is E=p^2/2m, so you see there's a quadratic term, and so that means p^2/2m=0.5kT. A simple harmonic oscillator has E=p^2/2m+0.5kx^2, so p^2/2m=0.5kT, 0.5kx^2=0.5kT, and E=kT. That's why it's called the "equipartition theorem", because the thermal energy is equally partitioned to every quadratic degree of freedom.