 
    
  
 
	If we let the energy of the ground state (  )
	be 0 (which we can do
	since we are free to set the zero of energy anywhere we want)
	then
 )
	be 0 (which we can do
	since we are free to set the zero of energy anywhere we want)
	then
	
  
 
The partition function is
  
 
so the entropy becomes
  
 
  
 
		For the ground state, we get P(0)=1/Z while for the
		excited state,   because the level is nondegenerate.
		Let us say that the probability of occupation of level 1
		is significant when the ratio
 
		because the level is nondegenerate.
		Let us say that the probability of occupation of level 1
		is significant when the ratio
		  becomes greater than 0.01.
		(This is arbitrary and we could have picked a different
		value.  The result would have been quantitatively
		different, but not qualitatively different.)
		Thus we want to know at what temperature
  becomes greater than 0.01.
		(This is arbitrary and we could have picked a different
		value.  The result would have been quantitatively
		different, but not qualitatively different.)
		Thus we want to know at what temperature
		
  
 
		By taking a natural logarithm of both sides of this
		equation and rearranging, we get
		  or
  or
		
  
 
This kind of calculation shows that an energy level only contributes significantly to the thermodynamic properties of a substance if its energy is comparable to kT.
  
 
The internal energy is therefore
  
 
Thus the entropy is
 