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04-BS-6 · May 2016

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).

Question 3: Spreader Beam — Combined Axial and Bending Stress (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.

Given.

QuantityValue
Hook load, P120 kN, at beam midspan
Cable geometryrise 1.6 m, horizontal run 2 m to each end connection plate
Connection-plate standoff0.12 m above the beam's top flange
SectionI-beam: flanges 140×30 mm, web 20 mm thick, clear web height 200 mm (overall depth 260 mm)
SteelFy = 350 MPa (normal), Fy,shear = 60 MPa, E = 200 GPa
1.6 m 0.12 m + c 2 m P = 120 kN 2 m 2 m Midspan section (cut here)
Spreader beam: cable geometry and eccentric pin standoff.
140 mm 30 mm 200 mm 30 mm 20 mm Beam cross-section
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.

  1. 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): $$V_{cable}=\frac{P}{2}=60\ \text{kN}\qquad T=\frac{V_{cable}}{1.6/L_c}=96.05\ \text{kN}$$ $$H = T\left(\frac{2.0}{L_c}\right) = 75.0\ \text{kN}\quad\text{(constant axial compression, both ends squeeze inward)}$$
  2. 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: $$M_{vert}=V_{cable}\left(\frac{4}{2}\right)=60(2)=120\ \text{kN}\cdot\text{m}$$
  3. 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): $$M_{ecc}=He=75.0(0.25)=18.75\ \text{kN}\cdot\text{m}\qquad M_{tot}=M_{vert}+M_{ecc}=138.75\ \text{kN}\cdot\text{m}$$
  4. Section properties. $$A=2(140)(30)+20(200)=12\,400\ \text{mm}^2\qquad I=\frac{140(260)^3-120(200)^3}{12}=1.2505\times10^{8}\ \text{mm}^4\qquad c=130\ \text{mm}$$
  5. (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.
  6. (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: $$Q_{NA}=140(30)(115)+20(100)(50)=5.83\times10^{5}\ \text{mm}^3$$ $$\tau_{max}=\frac{VQ_{NA}}{I\,t_w}=\frac{(60\,000)(5.83\times10^{5})}{(1.2505\times10^{8})(20)}=14.0\ \text{MPa} < 60\ \text{MPa}\quad\boxed{\text{OK}}$$
−150.3 MPa (top, compr.) +138.2 MPa (bot., tens.) N.A.′ Normal stress distribution
Normal stress distribution at midspan.
τmax = 14.0 MPa 0 0 Shear stress distribution
Shear stress distribution at midspan.
QuantityValue
Cable tension, T96.0 kN
Axial compression, H75.0 kN
Total midspan moment138.75 kN·m (120 vertical + 18.75 eccentric)
σtop (max compression)−150.3 MPa
σbot (max tension)+138.2 MPa
τmax at N.A.14.0 MPa