Elasticity — Question 6

Section 12-6 · Physics pages 1882–1883

Question 6 A shear pad separates lateral stiffness from normal compression A rectangular elastic pad has bonded face area A = .020 m2, thickness h = .050 m and shear modulus G = .80 MPa. Opposite tangential forces of 160 N act on its faces. Use uniform small shear: τ = Gγ, γ = ∆x/h. F F ∆x Shear deformation exaggerated; dashed outline shows the undeformed pad. (a) Find shear stress, strain and relative face displacement. (b) Find stored energy and the effect of doubling h at fixed force and area.
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Question 6 - Solution A shear pad separates lateral stiffness from normal compression F F ∆x (a) Derivation and calculation Uniform shear gives τ = F/A = 160/.020 = 8.00 kPa , γ = τ/G = 8000/(.80 × 106) = .0100 , ∆x = γh = .0100(.050) = .500 mm . (b) Result and interpretation The equivalent shear stiffness and stored energy are ks = GA/h = 3.20 × 105 N/m, U = 1 2F∆x = 1 2(160)(.000500) = .0400 J . At fixed F, A, G, doubling h gives k′ s = ks/2, ∆x′ = 2∆x = 1.00 mm and U′ = 2U = .0800 J. Stress and shear strain are unchanged. Physical check The computed shear strain is small, consistent with the stated linear small-shear model.

Question 6

A shear pad separates lateral stiffness from normal compression

A rectangular elastic pad has bonded face area A=.020m2A=.020\,\mathrm{m^2}, thickness h=.050mh=.050\,\mathrm m and shear modulus G=.80MPaG=.80\,\mathrm{MPa}. Opposite tangential forces of 160N160\,\mathrm N act on its faces. Use uniform small shear: τ=Gγ\tau=G\gamma, γ=Δx/h\gamma=\Delta x/h.

Diagram shown in the original SVG worksheet.

  1. Find shear stress, strain and relative face displacement.

  2. Find stored energy and the effect of doubling hh at fixed force and area.

Question 6 - Solution

A shear pad separates lateral stiffness from normal compression

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Uniform shear gives τ=F/A=160/.020=8.00kPa,\boxed{\tau=F/A=160/.020=8.00\ \mathrm{kPa}}, γ=τ/G=8000/(.80×106)=.0100,\boxed{\gamma=\tau/G=8000/(.80\times10^6)=.0100}, Δx=γh=.0100(.050)=.500mm.\boxed{\Delta x=\gamma h=.0100(.050)=.500\ \mathrm{mm}}.

(b) Result and interpretation

The equivalent shear stiffness and stored energy are ks=GA/h=3.20×105N/m,k_s=GA/h=3.20\times10^5\ \mathrm{N/m}, U=12FΔx=12(160)(.000500)=.0400J.\boxed{U=\tfrac12F\Delta x=\tfrac12(160)(.000500)=.0400\ \mathrm J}. At fixed F,A,GF,A,G, doubling hh gives ks′=ks/2k_s'=k_s/2, Δx′=2Δx=1.00\Delta x'=2\Delta x=1.00 mm and U′=2U=.0800U'=2U=.0800 J. Stress and shear strain are unchanged.

Physical check

The computed shear strain is small, consistent with the stated linear small-shear model.