Why divide by volume in lattice specific heat calculation

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dRic2
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Hi, I don't understand why the author in calculating the expression for the specific heat, divides by ##1/V## (the total volume).
Scanned printed textbook page with handwritten annotations showing statistical mechanics equations for phonon energy, including the specific heat expression C_V = (1/V) dE/dT with the 1/V circled in red, and the lattice result C_V = 3nNk integral over the density of states.


Also, in calculating the fraction of modes with frequency in the range ##v##, ##v+dv## he divides by ##V## (eq. 2.65, 2.67)

Printed textbook page showing Section 2.5 Lattice spectrum with equations 2.65 to 2.68 for the density of modes, with handwritten red annotations marking v_c = V/N and the prefactor v_c/(2π^3) and 1/(8π^3 N).
Thanks,
Ric
 
Energy is extensive (varies with system size), and dividing by another extensive quantity (volume) gives an intensive quantity. In this case, it’s volumetric heat capacity. Mass or molar heat capacity (where you divide the derivative of heat wrt temperature by mass or amount of substance) are more familiar, but it’s the same idea: you’re looking for a property which is independent of the size of the system.
 
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dRic2 said:
Also, in calculating the fraction of modes with frequency in the range v, v+dv he divides by V (eq. 2.65, 2.67)
The same as indicated by @TeethWhitener: The phonon density of states gives the number of modes per unit frequency per unit volume of real space.
 
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Thank you very much. I had to be sure because it was not explicitly specified, although it might be intuitive.