Skip to content

Physics · Ch 8 — Mechanical Properties of Solids

Bulk Modulus (K)

8.7

Bulk Modulus (K)

The bulk modulus, denoted KK, is the modulus of elasticity that applies to hydraulic (volume) stress and the corresponding volume strain -- the elastic constant governing how strongly a body resists a uniform change in its volume when subjected to a uniform pressure change over its entire surface, with no accompanying change in its overall shape. By Hooke's law, but with a deliberately inserted minus sign,

K=−ΔPΔV/VK = -\frac{\Delta P}{\Delta V/V}

where ΔP\Delta P is the (uniform) increase in pressure applied to the body and ΔV/V\Delta V/V is the resulting fractional change in its volume.

The minus sign here is not arbitrary -- it exists to keep KK itself a positive quantity for ordinary matter. Squeezing a body harder (increasing ΔP\Delta P, so ΔP>0\Delta P > 0) always makes its volume shrink (ΔV<0\Delta V < 0); without the minus sign, the ratio ΔP/(ΔV/V)\Delta P/(\Delta V/V) would itself always come out negative, which would be an awkward, unintuitive way to report an elastic constant that is supposed to represent how strongly a material resists compression. With the minus sign in place, KK comes out positive, and a larger value of KK correctly represents a material that resists compression more strongly (a smaller fractional volume change for a given pressure increase), matching the intuitive meaning shared by YY and η\eta.

The reciprocal of the bulk modulus is called the compressibility of the material, usually denoted CC (or sometimes β\beta or kk in other texts):

C=1KC = \frac{1}{K}

Compressibility directly measures how easily a material's volume changes under pressure -- a highly compressible material (large CC, small KK) shrinks readily under pressure, while a nearly incompressible material (small CC, large KK) barely shrinks at all, however hard it is squeezed. …