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2.14.1 Isotropic Materials
ОглавлениеThe situation simplifies when the material is linear thermoelastic and isotropic so that the stress-strain relations are
(2.157)
where E is Young’s modulus, ν is Poisson’s ratio, α is the thermal expansion coefficient and The inverse form is
(2.158)
When the stress field is hydrostatic so that σij=−pδij, and because σkk≡σ11+σ22+σ33, it follows from (2.157) that
(2.159)
The inverse form (2.158) may be written as
(2.160)
where λ and μ are Lamé’s constants, μ being the shear modulus, which can be calculated from Young’s modulus and Poisson’s ratio as follows:
(2.161)