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04-BS-6 · December 2013

Question 5 of 8: Statically Indeterminate Composite Axial Bar

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

Notes on this paper

National Exams December 2013 – 04-BS-6: Mechanics of Materials
3 hours duration, closed book (one hand-written aid sheet permitted). Any five of the eight questions constitute a complete paper; all eight are solved below as a complete study resource.

Reference texts: R.C. Hibbeler, Mechanics of Materials, 10th ed. (Ch. 5 torsion, Ch. 6 shear/moment diagrams & composite beams, Ch. 7 transverse shear, Ch. 8 combined loadings, Ch. 9 stress transformation, Ch. 12 deflection by integration, Ch. 13 buckling); F. Beer & E.R. Johnston, Mechanics of Materials; W. Gere & B. Goodno, Mechanics of Materials (alternates). A W-shape properties table printed on the exam's last page is not needed — every question supplies its own section dimensions.

Question 5: Statically Indeterminate Composite Axial Bar (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.

CuAlCuSteelP800 mm400 mmFig. Q5 – composite axial bar (statically indeterminate)
Composite bar: Al + 2×Cu in parallel (800 mm) in series with a steel bar (400 mm), pulled by P = 500 kN.

Given.

MemberA (mm2)E (GPa)fy (MPa)Length (mm)
Aluminum (1)120070400800
Copper (2, parallel)600 each100350800
Steel2500200350400

Applied load P = 500 kN, tension, at the free end.

Find. (a) The axial force carried by each bar. (b) The total horizontal displacement of the free end.

Approach. The steel bar is the only load path in its segment, so it carries the full 500 kN. In the left segment, the three parallel bars share the same rigid-plate displacement (compatibility); combine that with equilibrium (their forces must sum to 500 kN) to solve the once-indeterminate parallel system, then add the two segments' elongations.

  1. Steel segment (statically determinate). $$F_{steel}=P=500\ \text{kN}, \qquad \sigma_{steel}=\frac{500{,}000}{2500}=200\ \text{MPa} \ (< 350\ \text{MPa, OK})$$
  2. Parallel bundle: stiffness and compatibility. Each bar shares the same elongation $\delta$ over the common 800 mm length, so $F_i = k_i\delta$ with $k_i = A_iE_i/L$: $$k_{Al}=\frac{1200(70{,}000)}{800}=105{,}000\ \text{N/mm}, \qquad k_{Cu}=\frac{600(100{,}000)}{800}=75{,}000\ \text{N/mm (each)}$$ $$\Sigma k = 105{,}000+2(75{,}000)=255{,}000\ \text{N/mm}$$
  3. Solve for the shared elongation and each bar force. $$\delta = \frac{P}{\Sigma k}=\frac{500{,}000}{255{,}000}=1.961\ \text{mm}$$ $$F_{Al}=k_{Al}\delta = \boxed{205.9\ \text{kN}}, \qquad F_{Cu}=k_{Cu}\delta = \boxed{147.1\ \text{kN (each)}}$$ Check: $205.9+2(147.1)=500.0$ kN $=P$. σAl = 171.6 MPa ($<400$, OK); σCu = 245.1 MPa ($<350$, OK) — both bars remain elastic.
  4. Total end displacement. The steel segment's elongation adds in series to the (common) parallel-bundle elongation: $$\delta_{steel}=\frac{F_{steel}L_{steel}}{A_{steel}E_{steel}} =\frac{500{,}000(400)}{2500(200{,}000)}=0.400\ \text{mm}$$ $$\boxed{\delta_{total}=\delta_{left}+\delta_{steel}=1.961+0.400=2.361\ \text{mm}}$$

Final Results.

QuantityValue
FAl205.9 kN
FCu (each of 2)147.1 kN
Fsteel500.0 kN
δ of parallel bundle1.961 mm
δ of steel bar0.400 mm
Total end displacement2.361 mm