Elasticity — Question 8

Section 12-6 · Physics pages 1886–1887

Question 8 Axial stretching can leave volume nearly unchanged A slender isotropic specimen has E = 100 GPa and Poisson ratio ν = .30. Under uniaxial tensile stress 100 MPa, transverse surfaces are free. Use ϵ = σ/E and transverse strains ϵt = −νϵ. axial stretch Shape changes exaggerated; dashed outline is the unloaded specimen. (a) Find axial strain, fractional area change and fractional volume change to first order. (b) What volume change would the same axial strain produce if ν = .50, and does that imply zero elongation?
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Question 8 - Solution Axial stretching can leave volume nearly unchanged axial stretch (a) Derivation and calculation The axial and transverse strains are ϵ = σ/E = (100 × 106)/(100 × 109) = .00100 , ϵt = −νϵ = −.30(.00100) = −.000300. To first order, ∆A/A = 2ϵt = −.000600 , ∆V/V = ϵ + 2ϵt = (1 −2ν)ϵ = .000400 . (b) Result and interpretation At the same axial strain with ν = .50, ∆V/V = (1 −2(.50))ϵ = 0 . Nevertheless ∆L/L = ϵ = .00100̸ = 0. The transverse area contraction ∆A/A = −.00100 offsets elongation to first order, preserving volume while changing shape. Physical check The volume-change statement uses the specified small-strain approximation; zero volume strain does not imply zero axial strain.

Question 8

Axial stretching can leave volume nearly unchanged

A slender isotropic specimen has E=100GPaE=100\,\mathrm{GPa} and Poisson ratio ν=.30\nu=.30. Under uniaxial tensile stress 100MPa100\,\mathrm{MPa}, transverse surfaces are free. Use ϵ=σ/E\epsilon=\sigma/E and transverse strains ϵt=−νϵ\epsilon_t=-\nu\epsilon.

Diagram shown in the original SVG worksheet.

  1. Find axial strain, fractional area change and fractional volume change to first order.

  2. What volume change would the same axial strain produce if ν=.50\nu=.50, and does that imply zero elongation?

Question 8 - Solution

Axial stretching can leave volume nearly unchanged

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The axial and transverse strains are ϵ=σ/E=(100×106)/(100×109)=.00100,\boxed{\epsilon=\sigma/E=(100\times10^6)/(100\times10^9)=.00100}, ϵt=−νϵ=−.30(.00100)=−.000300.\epsilon_t=-\nu\epsilon=-.30(.00100)=-.000300. To first order, ΔA/A=2ϵt=−.000600,\boxed{\Delta A/A=2\epsilon_t=-.000600}, ΔV/V=ϵ+2ϵt=(1−2ν)ϵ=.000400.\boxed{\Delta V/V=\epsilon+2\epsilon_t=(1-2\nu)\epsilon=.000400}.

(b) Result and interpretation

At the same axial strain with ν=.50\nu=.50, ΔV/V=(1−2(.50))ϵ=0.\boxed{\Delta V/V=(1-2(.50))\epsilon=0}. Nevertheless ΔL/L=ϵ=.00100≠0\Delta L/L=\epsilon=.00100\ne0. The transverse area contraction ΔA/A=−.00100\Delta A/A=-.00100 offsets elongation to first order, preserving volume while changing shape.

Physical check

The volume-change statement uses the specified small-strain approximation; zero volume strain does not imply zero axial strain.