Question 3 of 8: Spreader Beam — Combined Axial and Bending Stress
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Exams May 2016 — 04-BS-6: Mechanics of Materials (3 hours, closed book,
one hand-written aid sheet permitted). Any FIVE of the eight questions constitute a complete
paper on the official exam; every question is answered below. A W-shape section-property table is attached at the end of the official exam; it is a red herring here — every question below supplies its own
built-up or standard section, and Question 2 cites the CISC-standard W610×125 properties
directly.
Reference texts: Hibbeler, Mechanics of Materials, 10th ed. (composite
beams, deflection by integration, combined loading, transformation of stress, columns, torsion,
shear/moment diagrams); CISC Handbook of Steel Construction (W-shape section properties).
Spreader beam: cable geometry and eccentric pin standoff.
Spreader-beam cross-section (I-beam).
Find. The normal-stress distribution (max & min) and the maximum shear
stress at the midspan cross-section.
Approach. Recognize that the two inclined cables do double duty: their VERTICAL
components act like simple end reactions (giving ordinary sagging bending), while their EQUAL and
opposite HORIZONTAL components squeeze the beam axially in compression. Because the cables attach
0.12 m above the beam's top flange (i.e. above the neutral axis), that axial force is applied
ECCENTRICALLY, adding a constant bending moment on top of the ordinary one. Superpose
$\sigma = -N/A \pm Mc/I$ at midspan, and use $\tau=VQ/(Ib)$ for the shear check.
Cable tension and its components. By symmetry each cable carries half the
120 kN vertical load. With rise 1.6 m and run 2.0 m (cable length $L_c=\sqrt{1.6^2+2.0^2}=2.561$ m):
$$V_{cable}=\frac{P}{2}=60\ \text{kN}\qquad T=\frac{V_{cable}}{1.6/L_c}=96.05\ \text{kN}$$
$$H = T\left(\frac{2.0}{L_c}\right) = 75.0\ \text{kN}\quad\text{(constant axial compression, both ends squeeze inward)}$$
Bending moment from the vertical components alone. The two 60 kN "reactions"
act exactly like a simply supported beam (span 4 m between the connection plates) carrying a
120 kN centre load:
$$M_{vert}=V_{cable}\left(\frac{4}{2}\right)=60(2)=120\ \text{kN}\cdot\text{m}$$
Extra moment from the eccentric axial force. Section centroid is $c=130$ mm
below the top flange; the connection plate stands a further 0.12 m above the flange, so the cable
line of action sits $e=0.12+0.130=0.25$ m above the neutral axis, at BOTH ends. An axial force
applied at the same eccentricity at both ends of a straight member is equivalent to the same force
through the centroid plus a CONSTANT moment $H\!\cdot\!e$, and here it adds in the SAME sense as
the sagging moment (both increase top compression, bottom tension):
$$M_{ecc}=He=75.0(0.25)=18.75\ \text{kN}\cdot\text{m}\qquad M_{tot}=M_{vert}+M_{ecc}=138.75\ \text{kN}\cdot\text{m}$$
(a) Combined normal stress at midspan (compression negative):
$$\sigma_{axial}=\frac{H}{A}=\frac{75\,000}{12\,400}=6.05\ \text{MPa (compression)}\qquad
\sigma_{bend}=\frac{M_{tot}\,c}{I}=\frac{(1.3875\times10^{8})(130)}{1.2505\times10^{8}}=144.24\ \text{MPa}$$
$$\sigma_{top}=-\sigma_{axial}-\sigma_{bend}=\boxed{-150.3\ \text{MPa (compression)}}\qquad
\sigma_{bot}=-\sigma_{axial}+\sigma_{bend}=\boxed{+138.2\ \text{MPa (tension)}}$$
Both are comfortably under the 350 MPa yield — the section is safe, and note the top/bottom
magnitudes DIFFER (150.3 vs 138.2 MPa) precisely because of the added axial term, which is exactly
why the question asks for max AND min separately rather than a single symmetric bending value.
(b) Maximum shear stress at the neutral axis, using the shear carried on this side
of midspan ($V=P/2=60$ kN) and the first moment of the half-section above the NA:
$$Q_{NA}=140(30)(115)+20(100)(50)=5.83\times10^{5}\ \text{mm}^3$$
$$\tau_{max}=\frac{VQ_{NA}}{I\,t_w}=\frac{(60\,000)(5.83\times10^{5})}{(1.2505\times10^{8})(20)}=14.0\ \text{MPa} < 60\ \text{MPa}\quad\boxed{\text{OK}}$$