Shear Modulus (G = τ/γ)

G=τγG = \frac{\tau}{\gamma}

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Shear strain γ is not a stretch but a change of angle: push the top of a block sideways by Δx while its height stays h, and γ = Δx/h, the small angle in radians by which the originally square corner has been racked out of true. The shear modulus is the stress needed per unit of that racking. Charles-Augustin de Coulomb measured it first, in the 1784 torsion-balance experiments that also gave him the law of electrostatics — he twisted fine wires and timed their oscillations. Steel runs G ≈ 77 GPa (11 600 ksi), aluminium ≈ 26 GPa. A shear stress of 60 MPa producing γ = 0.0008 rad implies G = 60 ÷ 0.0008 = 75 000 MPa = 75 GPa.

The trap is treating G as an independent property to look up separately: for an isotropic material it is locked to E and Poisson's ratio by E = 2G(1 + ν), so with ν ≈ 0.3 you always get G ≈ 0.385 E. Enter γ as a plain ratio (radians), not degrees — a shear strain of 0.001 is a milliradian, about 0.057°, and mixing the two inflates G by a factor of 57.

Shear Modulus (G = τ/γ)
G=τγG = \frac{\tau}{\gamma}
Where
  • GG= Shear modulus
  • τ\tau= Shear stress
  • γ\gamma= Shear strain (radians)
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