Elasticity — Question 4

Section 12-6 · Physics pages 1878–1879

Question 4 The effective area of a tapered rod is not its arithmetic mean A slender rod of length L and constant modulus E has slowly varying area A(x) = A0(1 + x/L). It carries axial tension F. In a one-dimensional small-strain model, a slice extends by dδ = F dx/[EA(x)]. F F A0 2A0 Longitudinal schematic of increasing area; the stated area law defines the model. (a) Integrate the extension and find the uniform area Aeff that gives the same extension. (b) Would replacing the rod by its arithmetic-mean area 3A0/2 overestimate or underestimate the extension?
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Question 4 - Solution The effective area of a tapered rod is not its arithmetic mean F F A0 2A0 (a) Derivation and calculation Integrate the local compliance: δ = F EA0 ∫L 0 dx 1 + x/L = FL ln 2 EA0 . Equating this to FL/(EAeff) gives Aeff= A0/ ln 2 = 1.443A0 . (b) Result and interpretation Using the arithmetic-mean area instead predicts δarith = FL E(3A0/2) = 2FL 3EA0 . Since 2/3 < ln 2, δarith < δ . The relative underestimate is 1 −2/(3 ln 2) = 3.82%. The narrow portions contribute disproportionately because compliance depends on 1/A. Physical check The effective area lies between A0 and 2A0, but below their arithmetic mean.

Question 4

The effective area of a tapered rod is not its arithmetic mean

A slender rod of length LL and constant modulus EE has slowly varying area A(x)=A0(1+x/L)A(x)=A_0(1+x/L). It carries axial tension FF. In a one-dimensional small-strain model, a slice extends by dδ=Fdx/[EA(x)]d\delta=F\,dx/[EA(x)].

Diagram shown in the original SVG worksheet.

  1. Integrate the extension and find the uniform area AeffA_{eff} that gives the same extension.

  2. Would replacing the rod by its arithmetic-mean area 3A0/23A_0/2 overestimate or underestimate the extension?

Question 4 - Solution

The effective area of a tapered rod is not its arithmetic mean

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Integrate the local compliance: δ=FEA0∫0Ldx1+x/L=FLln⁡2EA0.\delta=\frac{F}{EA_0}\int_0^L\frac{dx}{1+x/L} =\boxed{\frac{FL\ln2}{EA_0}}. Equating this to FL/(EAeff)FL/(EA_{\mathrm{eff}}) gives Aeff=A0/ln⁡2=1.443A0.\boxed{A_{\mathrm{eff}}=A_0/\ln2=1.443A_0}.

(b) Result and interpretation

Using the arithmetic-mean area instead predicts δarith=FLE(3A0/2)=2FL3EA0.\delta_{\mathrm{arith}}=\frac{FL}{E(3A_0/2)}=\frac{2FL}{3EA_0}. Since 2/3<ln⁡22/3<\ln2, δarith<δ.\boxed{\delta_{\mathrm{arith}}<\delta}. The relative underestimate is 1−2/(3ln⁡2)=3.82%1-2/(3\ln2)=3.82\%. The narrow portions contribute disproportionately because compliance depends on 1/A1/A.

Physical check

The effective area lies between A0A_0 and 2A02A_0, but below their arithmetic mean.