Answer:
The reason this general problem is so useful in a wide range of areas of physics is in physics we love to deal with harmonic approximations of systems.
The point of solving the problem of N harmonic oscillators in this way is that they approximate (actually, correspond to) the behaviour of the particles in an ideal gas.
Here, we work out the number of states (microstates) available to the system, the entropy of the system, and derive the energy of the corresponding ideal gas as a function of temperature.
QUESTION
The energy levels of a harmonic oscillator with frequency νν are given by
En=(n+12)ℏω,n=0,1,2,…(1)
(1)En=(n+12)ℏω,n=0,1,2,…
A system of NN uncoupled and distinguishable oscillators has the total energy
E=N2ℏω+Mℏω(2)
(2)E=N2ℏω+Mℏω
where MM is a non-negative integer.
Calculate the number ΩMΩM of states for a given E.
Calculate the entropy S=kBln(ΩM)S=kBln(ΩM) of the system using the Stirling formula for MM>>11 and NN>>11.
The temperature is defined as 1T=∂S∂E1T=∂S∂E. Express the total energy as a function of the temperature and discuss the function E(T)E(T).
Step-by-step explanation: