Using the generalized Gilvarry J. Appl. Phys. 28, 1253 (1957) equation of state, we show that for the case where the Murnaghan equation of state holds, partial deriv~(2)B/partial derivTpartial derivP=0 where B is the isothermal bulk modulus. This leads to the following results: (1) The product αBδ is independent of volume and pressure at constant temperature, where α=(partial deriv In V/partial derivT)_(P) and δ is the Anderson-Gruneisen parameter. (2) The isothermal bulk modulus can be separated into two functions, B(T,P)=B(T)+B(P), where B(T) is a function of temperature only and B(P) is a function of pressure only, (3) (partial derivIn(αB)/partial derivIn η)_(T)=-(partial derivIn δ/partial derivIn η)_(T). where η=V/V_(0). (4) (partial derivIn(αB)/partial derivP)_(T)=-(partial derivIn δ/partial derivP)_(T). (5) If ψ=δ, where ψ=(partial derivB/partial derivP)_(T), then δ is independent of pressure and volume.
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