216 SOLUTIONSwhere weused Substituting and from(S.4.93.21), we obtain a more general formula forAt constant volume (S.4.93.23) becomesthe same as before.4.94 Number Fluctuations (Colorado (a,b), Moscow
Phys-Tech (c))a) Using the formula derived in Problem 4.92, we haveConsider an assortment of particles which are in the quantum state.
They are statisticallyindependent of theother particles in thegas;therefore
we can apply (S.4.94.1) in the form
For a Fermi gas
So, by (S.4.94.2),