Conventions for the placement of axes in crystal elasticity
A good reference for the symmetry relation in the fourth-rank elasticity tensor () components is Brugger (1965), but it relies on a specific placement of Cartesian axes, which is unclear in the paper. A standard for the placement, though seems implicit now, is known by the ultrasound community, exists elsewhere.
R. N. Thurston (Truesdell, 1984):
By material coefficients, we here mean derivatives of a thermodynamic potential, evaluated at some generalized undistorted, zero-field state. In the simplest case, the only nonzero first derivative of any thermodynamic potential is its derivative with respect to the thermal variable, either temperature or entropy. A hydrostatic pressure at the undistorted state is permissible [cf. Sect. 11.4, especially Eq. (11.35)].
The elastic, dielectric, piezoelectric, and other coefficients of crystals are ordinarily specified with reference to a set of rectangular Cartesian axes that are chosen by convention. The conventional method of relating a set of rectangular axes to the crystallographic axes has been standardized through the work of Bond (1949) and others, and is described in publications of Mason (
19501947, 1966).
The original text in the book mistakenly refers to Mason (1950) instead of Mason (1947). The Bond (1949) one is a IRE (now IEEE) standard, the placement seems to be clear only in the 1949 version but not in more recent versions. Mason (1947) is a paper and should be quite easy to find; Mason (1966) is a book that seems to be difficult to find1.
A more recent reference is The AFLOW standard encyclopedia of crystallographic prototypes and its three relevant papers: Mehl et al., (2017), Hicks et al., (2019, 2021).
Reference
- Brugger, K. (1965). Pure Modes for Elastic Waves in Crystals. Journal of Applied Physics, 36(3), 759–768. https://doi.org/10.1063/1.1714215
- Mason, W. P. (1947). First and Second Order Equations for Piezoelectric Crystals Expressed in Tensor Form. Bell System Technical Journal, 26(1), 80–138. https://doi.org/10.1002/j.1538-7305.1947.tb01312.x
- Mason, W. P. (1950). Optical properties and the electro-optic and photoelastic effects in crystals expressed in tensor form. The Bell System Technical Journal, 29(2), 161–188. https://doi.org/10.1002/j.1538-7305.1950.tb00464.x
- Mason, W. P. (1966). Crystal Physics of Interaction Processes. Academic Press.
- Standards on Piezoelectric Crystals, 1949. (1949). Proceedings of the IRE, 37(12), 1378–1395. https://doi.org/10.1109/JRPROC.1949.229975
- Truesdell, C. (Ed.). (1984). Mechanics of Solids Volume IV: Waves in Elastic and Viscoelastic Solids (Theory and Experiment) (Vol. 4). Springer Berlin Heidelberg. https://link.springer.com/book/9783540131632
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Mason, W. P. graduates from Columbia University and held a visiting professor position in his late career until his retirement in 1977. ↩