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22-Mec-A7 Advanced Strength of Materials · December 2013

Question 1 of 7: Two-Segment Rod — Uniform Heating Between Rigid Supports

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

Notes on this paper

Paper format: National Exams, December 2013 — 07-Mech-A7 Advanced Strength of Materials. Open-book, 3 hours; any five of the seven problems constitute a complete paper and all problems are of equal value. All seven problems are solved as a study resource.

Reference texts. R.C. Hibbeler, Mechanics of Materials, 10th ed. (thermal & indeterminate axial members Ch. 4, plane stress/strain Ch. 9–10, energy methods Ch. 14); A.P. Boresi & R.J. Schmidt, Advanced Mechanics of Materials, 6th ed. (thick-walled cylinders Ch. 11, thin-walled open sections & torsional buckling Ch. 6&12); J.M. Gere & B.J. Goodno, Mechanics of Materials (strain rosettes, columns). Yield criteria follow the von Mises and Tresca formulations standard to these texts.

Question 1: Two-Segment Rod — Uniform Heating Between Rigid Supports (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.

Given. A two-segment rod A–B–C built in between rigid walls, both segments heated uniformly by ΔT = 60 °C.

Given data
Rod (1), A–BE1 = 135 GPa, A1 = 520 mm2, L1 = 120 mm, α1 = 7.5×10−6/°C
Rod (2), B–CE2 = 85 GPa, A2 = 950 mm2, L2 = 90 mm, α2 = 12.5×10−6/°C
Temperature riseΔT = +60 °C (both rods)
ConstraintRigid supports at A and C ⇒ total elongation = 0

Find. (a) the axial stresses σ1, σ2; (b) the direction and magnitude of the displacement of the welded joint B.

(1) (2) A B C L1 = 120 mm L2 = 90 mm Rigid support both ends; weld at B
Series rod fixed at A and C; heating induces a common internal force N (statically indeterminate).

Approach. The two rods carry the same internal force N (series equilibrium). Because both ends are held, the free thermal growth plus the mechanical (force) deformation of the pair must sum to zero — one compatibility equation gives N, hence the stresses; the motion of B is the net stretch of rod 1.

  1. Compatibility of the constrained pair. Free thermal expansion is cancelled by the flexibility of the two segments under the common force N: $$\alpha_1L_1\,\Delta T+\alpha_2L_2\,\Delta T+N\!\left(\frac{L_1}{A_1E_1}+\frac{L_2}{A_2E_2}\right)=0.$$
  2. Thermal and flexibility terms. Numerically, $$\alpha_1L_1\Delta T+\alpha_2L_2\Delta T=0.0540+0.0675=0.1215\ \text{mm},$$ $$\frac{L_1}{A_1E_1}+\frac{L_2}{A_2E_2}=1.709\times10^{-6}+1.115\times10^{-6}=2.824\times10^{-6}\ \tfrac{\text{mm}}{\text{N}}.$$
  3. Internal force. Solving, $$\boxed{N=-\frac{0.1215}{2.824\times10^{-6}}=-43.0\ \text{kN}}$$ negative ⇒ the constrained heating puts the rod pair into compression.
  4. Axial stresses (part a). The same force divides by each area: $$\sigma_1=\frac{N}{A_1}=\frac{-43\,025}{520}=-82.7\ \text{MPa},\qquad \sigma_2=\frac{N}{A_2}=\frac{-43\,025}{950}=-45.3\ \text{MPa}.$$ Both are compressive, the smaller-area rod (1) being the more highly stressed.
  5. Motion of joint B (part b). Measuring displacement positive toward C (right), B moves by the net elongation of rod 1: $$u_B=\alpha_1L_1\Delta T+N\frac{L_1}{A_1E_1}=0.0540-0.0736=\boxed{-0.0195\ \text{mm}}$$ The negative sign means B moves to the left by about 0.020 mm: rod 1 — the stiffer, lower-expansion segment — is compressed more than it thermally grows, so the weld is pulled back toward A. (Checking from the C side, rod 2's net change is +0.0195 mm, confirming the closure uA=uC=0.)
Results — Question 1
QuantityValue
Common internal force N−43.0 kN (compression)
Stress in rod (1), σ1−82.7 MPa
Stress in rod (2), σ2−45.3 MPa
Displacement of joint B0.0195 mm to the left
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