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Symmetry Constraints on Properties

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Crystallography and Crystal Chemistry
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Abstract

This chapter introduces the distinction between isotropic and anisotropic properties as well as the application of coordinate transformations to solve problems involving anisotropic properties. Neumann’s Principle and the Curie Principle are also discussed.

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Notes

  1. 1.

    They are often called the Curie Laws although they are not, strictly speaking, laws and Curie himself spoke only of “les propositions” of symmetry.

  2. 2.

    For the more mathematically pedantic, a tensor is often thought of as a generalized matrix. While any rank-two tensor can be represented as a matrix, not every matrix is really a rank-two tensor. A matrix consists of the coefficients of a (1,1) tensor, but it is not a tensor itself.

  3. 3.

    In Einstein summation notation, a summation is implied over every subscript which appears twice on the same side of an equation (m, n, o, and p in this case).

Works Cited

  1. F. E. Neumann, Vorlesungen über die Theorie der Elastizität der festen Körper und des Lichtäthers, O. E. Meyer, Ed., Leipzig: B. G. Teubner-Verlag, 1885.

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  2. P. Curie, “Sur la symétrie dans les phénomènes physiques, symétrie d’un champ électrique et d’un champ magnétique,” Journal de Physique Theorique et Appliquee, vol. 3, pp. 393–415, 1894.

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Review Questions

Review Questions

  1. 1.

    Briefly explain the Curie Principle.

  2. 2.

    An object with point symmetry \( m\overline{3}m \) (Oh) distorts under uniaxial stress along [001]. What is the point group of the distorted object? What is it when the stress is along [111]? If an applied electric field removes the centre of symmetry in each case, to which point groups would the distorted objects now belong?

  3. 3.

    Carbon atoms in graphite are bonded within (001) via strong triangular (120°) sp2 hybrid σ bonding. The remaining unbonded 2p electrons form delocalized π bonds, and the adjacent sheets are held together by weak Van der Waals forces. For this reason, both the electrical and thermal conductivities of graphite are higher in the (001) than normal to it.

    The thermal conductivity kij is a tensor that relates the heat flux h to the temperature gradient dT/dx according to:

$$ {h}_i={k}_{ij}\frac{dT}{dx_j} $$

The thermal conductivity tensor of graphite is:

$$ {k}_{ij}=\left|\begin{array}{ccc}355& 0& 0\\ {}0& 355& 0\\ {}0& 0& 89\end{array}\right|\kern0.5em {\mathrm{Wm}}^{-1}\;{\mathrm{K}}^{-1} $$
  1. (a)

    If a gradient of 100 K/m is applied along the y direction, what is the resulting heat flow (in kW/m2)?

  2. (b)

    If a gradient of 100 K/m is applied along the z direction, what is the resulting heat flow (in kW/m2)?

  1. 4.

    Explain how Fourier’s Law, Ohm’s Law, and Fick’s Laws of Diffusion are related.

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Cite this chapter

Ubic, R. (2024). Symmetry Constraints on Properties. In: Crystallography and Crystal Chemistry. Springer, Cham. https://doi.org/10.1007/978-3-031-49752-0_12

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