Question 1 of 8: Rigid Bar on a Pin and Two Cables
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Exams May 2014 – 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 wide-flange (W-shape) properties
table printed on the exam's last page supplies the section used in Question 8.
Question 1: Rigid Bar on a Pin and Two Cables (20 marks)
Rigid bar ABCD: pin at A, cables at B (3 m) and C (7 m), triangular load 0→80 kN/m from A to D.
Given.
Quantity
Value
Spacing A–B–C–D
4 m, 4 m, 4 m (12 m total)
Pin at A
30 mm diameter, double shear
Cable diameter (B and C)
25 mm
Cable lengths
LB = 3 m, LC = 7 m
Cable E, fy
200 GPa, 800 MPa
Triangular load
0 at A, rising to 80 kN/m at D
Find. (a) Cable forces TB, TC; (b) the vertical
displacement at D; (c) the shear stress in the double-shear pin at A.
Approach. The rigid bar is held by one pin and two cables — four
reaction unknowns (Ax, Ay, TB, TC) against three
equilibrium equations, so the bar is indeterminate to one degree; close it with a rigid-body
rotation compatibility equation relating the two cable elongations, then finish with statics.
Resultant of the triangular load. $$W = \tfrac12(80)(12) = 480\ \text{kN},
\qquad \bar x = \tfrac23(12) = 8\ \text{m from A (i.e. directly over C)}$$
Compatibility. The bar is rigid and pinned at A, so it rotates by a single
small angle θ about A; the vertical drop at B and C equals the cable elongations
$\delta_B=4\theta$, $\delta_C=8\theta$, giving $\delta_C = 2\delta_B$. With
$\delta = TL/(AE)$ (same A, E for both cables):
$$\frac{T_C(7)}{AE} = 2\,\frac{T_B(3)}{AE} \ \Rightarrow\ T_C = \frac{6}{7}T_B$$
Moment equilibrium about A. $$T_B(4) + T_C(8) = W\bar x = 480(8) = 3840\
\text{kN}\cdot\text{m}$$ Substituting $T_C=\tfrac67 T_B$:
$$T_B\!\left(4+\tfrac{48}{7}\right)=3840 \ \Rightarrow\
\boxed{T_B = 353.7\ \text{kN}}, \qquad \boxed{T_C = \tfrac67(353.7)=303.2\ \text{kN}}$$
(b) Displacement at D. $$\delta_B=\frac{T_B L_B}{A_{cable}E}=
\frac{353{,}700(3000)}{490.9(200{,}000)}=10.81\ \text{mm}, \qquad
\theta=\frac{\delta_B}{4000}=2.702\times10^{-3}\ \text{rad}$$
$$\boxed{\delta_D = 12{,}000\,\theta = 32.4\ \text{mm, downward}}$$
(check: $\delta_C=8000\theta=21.6$ mm $=T_C L_C/(A_{cable}E)$, confirming compatibility).
(c) Pin shear at A. Vertical equilibrium of the bar (up positive):
$$A_y + T_B + T_C - W = 0 \ \Rightarrow\ A_y = 480-353.7-303.2=-176.8\ \text{kN}$$
i.e. the pin must pull DOWN 176.8 kN on the bar (the two cables together over-carry the
distributed load, so the pin supplies the balancing downward force). With double shear
($A_{pin}=\tfrac{\pi}{4}(30)^2=706.9\ \text{mm}^2$, two shear planes):
$$\boxed{\tau_{pin} = \frac{V}{2A_{pin}} = \frac{176{,}800}{2(706.9)} =
125.1\ \text{MPa}}$$