Birch–Murnaghan equation of state

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Template:Short description Template:Confusion The Birch–Murnaghan isothermal equation of state, published in 1947 by Albert Francis Birch of Harvard,<ref name=Birch47>Template:Cite journal</ref> is a relationship between the volume of a body and the pressure to which it is subjected. Birch proposed this equation based on the work of Francis Dominic Murnaghan of Johns Hopkins University published in 1944,<ref name=Murn44>Template:Cite journal</ref> so that the equation is named in honor of both scientists.

Expressions for the equation of state

The third-order Birch–Murnaghan isothermal equation of state is given by <math display="block"> P(V)=\frac{3B_0}{2} \left[\left(\frac{V_0}{V}\right)^{7/3} - \left(\frac{V_0}{V}\right)^{5/3}\right] \left\{1+\frac{3}{4}\left(B_0^\prime-4\right) \left[\left(\frac{V_0}{V}\right)^{2/3} - 1\right]\right\}. </math> where P is the pressure, V0 is the reference volume, V is the deformed volume, B0 is the bulk modulus, and B0' is the derivative of the bulk modulus with respect to pressure. The bulk modulus and its derivative are usually obtained from fits to experimental data and are defined as <math display="block"> B_0 = -V \left(\frac{\partial P}{\partial V}\right)_{P = 0}</math> and <math display="block">B_0' = \left(\frac{\partial B}{\partial P}\right)_{P = 0}</math> The expression for the equation of state is obtained by expanding the Helmholtz free energy in powers of the finite strain parameter f, defined as <math display="block">f = \frac{1}{2}\left[\left(\frac{V_0}{V}\right)^Template:2/3 - 1\right] \,,</math> in the form of a series.<ref name=Poirier>Template:Cite book</ref>Template:Rp This is more evident by writing the equation in terms of f. Expanded to third order in finite strain, the equation reads,<ref name=Poirier/>Template:Rp <math display="block"> P(f) = 3 B_0 f (1 + 2 f)^{5/2} ( 1 + a f + \mathit{higher~order ~terms})\,, </math> with <math> a = \frac{3}{2}(B_0' - 4) </math>.

The internal energy, Template:Math, is found by integration of the pressure: <math display="block"> E(V) = E_0 + \frac{9V_0B_0}{16} \left\{ \left[\left(\frac{V_0}{V}\right)^{2/3} - 1\right]^3 B_0^\prime + \left[\left(\frac{V_0}{V}\right)^{2/3} - 1\right]^2 \left[6-4\left(\frac{V_0}{V}\right)^{2/3}\right]\right\}. </math>

See also

References

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