Specific quantity

An intensive quantity formed by dividing an extensive variable by an extensive reference amount (mass, particle number, or volume).
Specific quantity

A specific quantity is a “per-unit-amount” version of an . Dividing by an appropriate extensive reference makes the result independent of system size (for homogeneous systems), so specific quantities are typically .

Let XX be an and let Y>0Y>0 be an extensive reference measure of system size (commonly mass mm, NN, or VV). The specific quantity of XX per YY is

xXY. x \equiv \frac{X}{Y}.

When the system is homogeneous (no macroscopic gradients), scaling the system by a factor λ\lambda multiplies both XX and YY by λ\lambda, so the ratio xx is unchanged; this is why xx behaves as an .

Physical interpretation

Specific quantities encode material properties “per unit amount,” which is often what experiments control or what constitutive laws use. For example, energy per particle compares energetic content to the number of particles present, while energy per volume compares energetic content to occupied space.

Common thermodynamic examples

  • Per particle: U/NU/N (specific internal energy per particle), S/NS/N (entropy per particle).
  • Per volume (densities): N/VN/V, U/VU/V, S/VS/V.
  • Per mass (common engineering usage): U/mU/m, S/mS/m, and the specific volume V/mV/m.

Key property: weighted averaging under composition

If a system is partitioned into two parts AA and BB with the same definition of x=X/Yx=X/Y, then

xtot=XA+XBYA+YB=YAYA+YBxA+YBYA+YBxB. x_{\text{tot}}=\frac{X_A+X_B}{Y_A+Y_B} = \frac{Y_A}{Y_A+Y_B}\,x_A+\frac{Y_B}{Y_A+Y_B}\,x_B.

So a specific quantity is an average of subsystem values weighted by the reference amount YY.