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22-Mec-A7 Advanced Strength of Materials · May 2016

Question 1 of 8: Truss member forces by an energy method

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

Notes on this paper

Paper format: National Exams — May 2016, 07-Mec-A7 Advanced Strength of Materials. Open-book, 3 hours, eight problems of equal value; any five constitute a complete paper. All eight are solved as a study resource.

Reference texts. A.P. Boresi & R.J. Schmidt, Advanced Mechanics of Materials, 6th ed. (Wiley); A.C. Ugural & S.K. Fenster, Advanced Strength and Applied Elasticity, 4th ed. (Prentice Hall); R.C. Hibbeler, Mechanics of Materials, 10th ed. (Pearson); J.M. Gere & B.J. Goodno, Mechanics of Materials, 9th ed. All symbols follow the paper’s notation.

Question 1: Truss member forces by an energy method (equal value)

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 pin-jointed truss with top chord E–F–G and bottom chord A–B–C–D. Verticals EA, FB, GC and diagonals AF, FC, GD; every horizontal and vertical member is 1 m, so each diagonal is √2 m at 45°. Support A is a pin, B and C are rollers; D is a free (loaded) joint. Loads: 10 kN horizontal at E, 17 kN vertical (down) at D.

Find. The axial forces in members FG, GD and CD (tension positive).

EFG ABCD 10 kN 17 kN
Truss geometry (each grid bay 1 m). Members FG, GD (diagonal) and CD lie in the right-hand panel between the roller at C and the free loaded joint D.

Approach. Although the complete frame is one degree statically indeterminate (m + r = 15 > 2j = 14), the three requested bars lie in the right panel, which is reached by isolating the free joint D and then joint G. These joints are internally determinate, so equilibrium fixes FG, GD and CD exactly — and Castigliano’s theorem (minimum strain energy) returns the same values because the single redundancy sits in the closed left/central bays and induces no force in these members.

  1. Isolate joint D (members CD, GD and the 17 kN load). GD rises to G at 45°. Vertical equilibrium gives the diagonal force: $$\sum F_y = 0:\quad F_{GD}\sin45^\circ - 17 = 0 \;\Rightarrow\; F_{GD} = \frac{17}{\sin45^\circ} = 17\sqrt2$$ $$\boxed{F_{GD} = 24.04\ \text{kN (tension)}}$$
  2. Horizontal equilibrium at D gives CD. The diagonal pulls D up-and-left, so the bottom chord must push back: $$\sum F_x = 0:\quad -F_{CD} - F_{GD}\cos45^\circ = 0 \;\Rightarrow\; F_{CD} = -17\sqrt2\cos45^\circ = -17$$ $$\boxed{F_{CD} = 17\ \text{kN (compression)}}$$
  3. Move to joint G (members FG, GC, GD). With GD now known, horizontal equilibrium gives the top-chord force: $$\sum F_x = 0:\quad -F_{FG} + F_{GD}\cos45^\circ = 0 \;\Rightarrow\; F_{FG} = 17\sqrt2\cos45^\circ = 17$$ $$\boxed{F_{FG} = 17\ \text{kN (tension)}}$$ (Vertical equilibrium at G additionally gives the vertical GC = 17 kN compression, a useful check.)
  4. Confirm the 10 kN load does not enter these bars. The horizontal 10 kN at E is carried leftward into the pin at A through chord EF and the left diagonal; it produces no force in the right-panel members FG, GD, CD, whose values depend only on the 17 kN tip load. A unit-load (virtual-work) check with a 1 kN dummy applied along each of these bars reproduces the same forces, confirming the energy method and equilibrium agree.
Question 1 — member forces
MemberForceSense
FG17.0 kNTension
GD17√2 = 24.04 kNTension
CD17.0 kNCompression
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