Elasticity — Question 1

Section 12-6 · Physics pages 1872–1873

Question 1 A measurement offset must not be mistaken for material compliance A wire has unloaded length L = 2 m and area A = 5 mm2. Its extension gauge reads .30 mm at 100 N and .70 mm at 300 N. In this range the wire is linear elastic, but the gauge has an unknown constant zero offset b: r = FL/(EA) + b. F (N) r (mm) 100 .30 300 .70 Gauge reading versus applied force; the extrapolated intercept need not be zero. (a) Infer Young's modulus without assuming the gauge zero is correct. (b) Find b and the true extension at 100 N.
Show solutionHide solution
Question 1 - Solution A measurement offset must not be mistaken for material compliance F (N) r (mm) 100 .30 300 .70 (a) Derivation and calculation Taking differences eliminates the constant offset: ∆r ∆F = L EA = (.70 −.30)10−3 300 −100 = 2.00 × 10−6 m/N. Thus E = 2 (5 × 10−6)(2 × 10−6) = 200 GPa . (b) Result and interpretation The true extension at 100 N is δ100 = 100(2 × 10−6) = .200 mm . Hence b = r100 −δ100 = .300 −.200 = .100 mm . At 300 N the model predicts .600 + .100 = .700 mm, recovering the other reading. Physical check The modulus depends on the slope of the force–extension relation, so a constant gauge offset does not affect it.

Question 1

A measurement offset must not be mistaken for material compliance

A wire has unloaded length L=2mL=2\,\mathrm m and area A=5mm2A=5\,\mathrm{mm^2}. Its extension gauge reads .30mm.30\,\mathrm{mm} at 100N100\,\mathrm N and .70mm.70\,\mathrm{mm} at 300N300\,\mathrm N. In this range the wire is linear elastic, but the gauge has an unknown constant zero offset bb: r=FL/(EA)+br=FL/(EA)+b.

Diagram shown in the original SVG worksheet.

  1. Infer Young's modulus without assuming the gauge zero is correct.

  2. Find bb and the true extension at 100N100\,\mathrm N.

Question 1 - Solution

A measurement offset must not be mistaken for material compliance

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Taking differences eliminates the constant offset: ΔrΔF=LEA=(.70−.30)10−3300−100=2.00×10−6m/N.\frac{\Delta r}{\Delta F}=\frac{L}{EA} =\frac{(.70-.30)10^{-3}}{300-100}=2.00\times10^{-6}\ \mathrm{m/N}. Thus E=2(5×10−6)(2×10−6)=200GPa.\boxed{E=\frac{2}{(5\times10^{-6})(2\times10^{-6})}=200\ \mathrm{GPa}}.

(b) Result and interpretation

The true extension at 100 N is δ100=100(2×10−6)=.200mm.\boxed{\delta_{100}=100(2\times10^{-6})=.200\ \mathrm{mm}}. Hence b=r100−δ100=.300−.200=.100mm.\boxed{b=r_{100}-\delta_{100}=.300-.200=.100\ \mathrm{mm}}. At 300 N the model predicts .600+.100=.700.600+.100=.700 mm, recovering the other reading.

Physical check

The modulus depends on the slope of the force–extension relation, so a constant gauge offset does not affect it.