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)
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).
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.
Isolate joint D (members CD, GD and the 17 kN load). GD rises to G at 45°. Vertical equilibrium gives the diagonal force:
$$\sum F_y = 0:\quad F_{GD}\sin45^\circ - 17 = 0 \;\Rightarrow\; F_{GD} = \frac{17}{\sin45^\circ} = 17\sqrt2$$
$$\boxed{F_{GD} = 24.04\ \text{kN (tension)}}$$
Horizontal equilibrium at D gives CD. The diagonal pulls D up-and-left, so the bottom chord must push back:
$$\sum F_x = 0:\quad -F_{CD} - F_{GD}\cos45^\circ = 0 \;\Rightarrow\; F_{CD} = -17\sqrt2\cos45^\circ = -17$$
$$\boxed{F_{CD} = 17\ \text{kN (compression)}}$$
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.)
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.