Relationship between bulk modulus and elastic constant

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The discussion focuses on the relationship between bulk modulus (B) and elastic constants (Cij), highlighting that the equation B = Cij/9 may not apply universally, particularly for materials with lower symmetry. The correct relationship for polycrystalline isotropic cubic crystals is B = 1/3 (C11 + 2*C12). For non-cubic materials, different averaging methods, such as Voigt and Reuss averages, can be used to derive bulk modulus from elastic constants. The significant discrepancy between the calculated bulk modulus values suggests that the material's structure may not conform to the assumptions of the simpler models. Understanding the specific material characteristics is essential for accurate calculations.
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I am getting the bulk modulus from fitting the equation of states and calculating the elastic constant. It seems that there is some relationship between bulk modulus B and elastic constant Cij, B=Cij/9,where i,j run from 1 to 3.
But my result is far away from this, say B=50 from fitting EOS and B=300 from elastic constant. Is this resonable or B=Cij/9 cann't be applied to some material(structure)?

Thanks a lot!
 
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The relationship between the bulk modulus and the elastic constants is:

B = 1/3 (C11 + 2*C12) for polycrystalline, isotropic cubic crystals

If the material has lower symmetry like a orthorhombic material it would have more independent elastic constants. Remember the concept of the bulk modulus was developed for polycrystalline material only. Not that single crystals don't resist volumetric distortion - of course they do. This resistance is going to be system specific and to give further details I need more info.

Regards

Modey3
 
To add, if the system is not cubic, there are two possibilities for the polycrystalline Bulk Modulus from the elastic constants.

Voight Average:

9B = ( c11 + c22 + c33 ) + 2*(c12 + c13 + c23)

Reuss Average

1/B = ( s11 + s22 + s33 ) + 2*(s12 + s13 + s23);

Details in the paper

"The Elastic Behaviour of a Crystalline Aggregate", by R.Hill.

Proceedings of the Physical Society of London, Section A. Vol 65, No 5. May 1952,pp349-354.
 
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