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22-Mec-A7 Advanced Strength of Materials · December 2017

Question 3 of 8: Semicircular Curved Beam by Castigliano’s Theorem

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format. National Exams, December 2017 — 16-Mec-A7 Advanced Strength of Materials. Open-book, 3 hours; any five of eight problems constitute a complete paper (all problems of equal value). All eight problems are solved as a study resource.

Reference texts. Boresi & Schmidt, Advanced Mechanics of Materials (6th); Ugural & Fenster, Advanced Mechanics of Materials and Applied Elasticity (5th); Timoshenko & Goodier, Theory of Elasticity (3rd); Hibbeler, Mechanics of Materials (10th).

Question 3: Semicircular Curved Beam by Castigliano’s Theorem (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

A P B R = 500 mm
Q3. Semicircular curved beam, mean radius R = 500 mm, fixed at B, horizontal load P at the free end A.

Given. A semicircular beam fixed at B, loaded by a horizontal force $P$ at the free end A.

Given data
Mean radius$R = 500\ \text{mm}$
Second moment of area$I = 810\times10^{6}\ \text{mm}^4$
Modulus$E = 200\ \text{GPa}$, so $EI=1.62\times10^{14}\ \text{N}\cdot\text{mm}^2$
Horizontal deflection limit$\delta_H \le 0.1\ \text{mm}$

Find. (a) allowable $P$; (b) magnitude and direction of the vertical deflection at A.

Approach. For a slender curved beam only bending energy is significant. Parametrize the arc by the polar angle $\theta$ (from B at $\theta=0$ to A at $\theta=\pi$); write $M(\theta)$ from the end loads and apply Castigliano, using a dummy vertical load $Q$ at A for the vertical component.

  1. Bending moment. A section at angle $\theta$ carries only the end load $P$ (horizontal, at A): $M(\theta)=-P R\sin\theta$. Adding a dummy vertical $Q$ at A gives $M=-PR\sin\theta-QR(1+\cos\theta)$.
  2. Horizontal deflection (Castigliano). With $ds=R\,d\theta$ and $\partial M/\partial P=-R\sin\theta$, $$\delta_H=\frac{1}{EI}\int_0^{\pi}\!M\frac{\partial M}{\partial P}R\,d\theta=\frac{PR^3}{EI}\int_0^{\pi}\sin^2\theta\,d\theta=\frac{\pi P R^3}{2EI}.$$
  3. Allowable force (part a). Setting $\delta_H=0.1\ \text{mm}$: $$P=\frac{2EI\,\delta_H}{\pi R^3}=\frac{2(1.62\times10^{14})(0.1)}{\pi(500)^3}=\boxed{82.5\ \text{kN}}$$
  4. Vertical deflection (part b). With $\partial M/\partial Q=-R(1+\cos\theta)$ evaluated at $Q=0$, $$\delta_V=\frac{1}{EI}\int_0^{\pi}\!(-PR\sin\theta)\bigl[-R(1+\cos\theta)\bigr]R\,d\theta=\frac{2PR^3}{EI}.$$
  5. Evaluate. $\delta_V=\dfrac{2(82\,500)(500)^3}{1.62\times10^{14}}=\boxed{0.127\ \text{mm, directed upward}}$ (the $+Q$ sense), i.e. $\delta_V=\tfrac{4}{\pi}\delta_H$.
Results — curved-beam deflection
QuantityValue
Allowable force $P$ (for $\delta_H=0.1$ mm)82.5 kN
Vertical deflection $\delta_V$0.127 mm, upward
Check: Only bending strain energy is retained; axial and shear contributions scale as $(\text{section depth}/R)^2$ and are negligible for this slender arc. The two closed-form results were cross-checked by numerical integration of the virtual-work integrals.