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Template:Elastic moduli

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Homogeneous isotropic linear elastic materials have their elastic properties uniquely determined by any two quantities among these; thus, given any two, any other of the elastic moduli can be calculated according to these formulas, provided both for 3D materials (first part of the table) and for 2D materials (second part).
3D Formulae
Knowns Bulk modulus (K) Young's modulus (E) Lamé's first parameter (λ) Shear modulus (G) Poisson's ratio (ν) P-wave modulus (M) Notes
(K, E) 3KE/3 − E/3K E/3 − E/3K 1/2E/6K 3K + E/3 − E/3K
(K, λ) 9K(K − λ)/3K − λ 3(K − λ)/2 λ/3K − λ 3K − 2λ
(K, G) 9KG/3K + G K2G/3 3K − 2G/6K + 2G K + 4G/3
(K, ν) 3K(1 − 2ν) 3/1 + ν 3K(1 − 2ν)/2(1 + ν) 3K(1 − ν)/1 + ν
(K, M) 9K(MK)/3K + M 3KM/2 3(MK)/4 3KM/3K + M
(E, λ) E + 3λ + R/6 E − 3λ + R/4 E + R/1/4 E − λ + R/2 R = ±(E2 + 9λ2 + 2Eλ)1/2
(E, G) EG/3(3GE) G(E − 2G)/3GE E/2G − 1 G(4GE)/3GE
(E, ν) E/3 − 6ν /(1 + ν)(1 − 2ν) E/2(1 + ν) E(1 − ν)/(1 + ν)(1 − 2ν)
(E, M) 3ME + S/6 ME + S/4 3M + ES/8 E + S/4M1/4 S = ±(E2 + 9M2 − 10EM)1/2
(λ, G) λ + 2G/3 G(3λ + 2G)/λ + G λ/2(λ + G) λ + 2G
(λ, ν) λ/3(1 + 1/v) λ(1/ν − 2ν − 1) λ(1/2ν − 1) λ(1/ν − 1)
(λ, M) M + 2λ/3 (M − λ)(M+2λ)/M + λ M − λ/2 λ/M + λ
(G, ν) 2G(1 + ν)/3 − 6ν 2G(1 + ν) 2 G ν/1 − 2ν 2G(1 − ν)/1 − 2ν
(G, M) M4G/3 G(3M − 4G)/MG M − 2G M − 2G/2M − 2G
(ν, M) M(1 + ν)/3(1 − ν) M(1 + ν)(1 − 2ν)/1 − ν M ν/1 − ν M(1 − 2ν)/2(1 − ν)
2D Formulae
Knowns (K) (E) (λ) (G) (ν) (M) Notes
(K2D, E2D) 2K2D(2K2DE2D)/4K2DE2D K2DE2D/4K2DE2D 2K2DE2D/2K2D 4K2D^2/4K2DE2D
(K2D, λ2D) 4K2D(K2D − λ2D)/2K2D − λ2D K2D − λ2D λ2D/2K2D − λ2D 2K2D − λ2D
(K2D, G2D) 4K2DG2D/K2D + G2D K2DG2D K2DG2D/K2D + G2D K2D + G2D
(K2D, ν2D) 2K2D(1 − ν2D) 2K2Dν2D/1 + ν2D K2D(1 − ν2D)/1 + ν2D 2K2D/1 + ν2D
(E2D, G2D) E2DG2D/4G2DE2D 2G2D(E2D − 2G2D)/4G2DE2D E2D/2G2D − 1 4G2D^2/4G2DE2D
(E2D, ν2D) E2D/2(1 − ν2D) E2Dν2D/(1 + ν2D)(1 − ν2D) E2D/2(1 + ν2D) E2D/(1 + ν2D)(1 − ν2D)
2D, G2D) λ2D + G2D 4G2D2D + G2D)/λ2D + 2G2D λ2D/λ2D + 2G2D λ2D + 2G2D
2D, ν2D) λ2D(1 + ν2D)/2ν2D λ2D(1 + ν2D)(1 − ν2D)/ν2D λ2D(1 − ν2D)/2ν2D λ2D/ν2D
(G2D, ν2D) G2D(1 + ν2D)/1 − ν2D 2G2D(1 + ν2D) 2 G2D ν2D/1 − ν2D 2G2D/1 − ν2D
(G2D, M2D) M2DG2D 4G2D(M2DG2D)/M2D M2D − 2G2D M2D − 2G2D/M2D