In Ashcroft and Mermin Chapter 1, just above equation (1.50) and in the context of a classical ideal electron gas, it is said that the electronic specific heat at constant volume $c_v$ is defined by
$$c_v=\frac{\frac{dE}{dT}}{V}$$
which seemed highly irregular to me (I would have expected division by the mass $M$ of the system of electrons). Is there any reason for this that I am perhaps missing?