Question 7 of 8: I-Beam Cantilever – Bending and Shear Stress
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Exams December 2013 – 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 W-shape properties table printed on
the exam's last page is not needed — every question supplies its own section dimensions.
Cantilever I-beam, 35 kN at the 4 m tip; section 200×300 mm overall, 10 mm flanges, 15 mm web.
Given.
Quantity
Value
Length, tip load
4 m, 35 kN
Flanges
200 mm × 10 mm (top and bottom)
Web
15 mm thick, 280 mm clear height
Overall depth
300 mm
Allowable σ / τ
240 MPa / 60 MPa
Find. (a) Maximum absolute normal and shear stress in the beam. (b) The shear
stress at point E (outer tip of the bottom flange), with justification.
Approach. Compute I by parallel-axis composition of the web and two flanges;
the maximum moment and constant shear both occur at the fixed base; use $\sigma=Mc/I$ and
$\tau=VQ/(It)$ at the neutral axis; argue point E from the free-surface condition.
Section properties (about the strong axis).
$$I_{web}=\frac{15(280)^3}{12}=27.44\times10^6\ \text{mm}^4$$
$$I_{flange}= \frac{200(10)^3}{12}+200(10)(145)^2 = 42.07\times10^6\ \text{mm}^4\ \text{(each,
about the NA, }d=145\text{ mm)}$$
$$I = I_{web}+2I_{flange} = \boxed{111.6\times10^6\ \text{mm}^4}, \qquad c=150\ \text{mm}$$
Maximum normal stress. Fixed-end moment $M=35(4)=140$ kN·m
(hogging, maximum at the wall since it is a single tip load with no other loading):
$$\sigma_{max}=\frac{Mc}{I}=\frac{140\times10^6(150)}{111.6\times10^6}
=\boxed{188.2\ \text{MPa}}\quad(<240\ \text{MPa allowable, OK})$$
Maximum shear stress (at the neutral axis). $V=35$ kN throughout (single
tip load, no distributed load). First moment of the area above the NA:
$$Q=A_{flange}\,d_{flange} + \left(t_w\cdot\frac{h_w}{2}\right)\frac{h_w}{4}
=2000(145)+(15\times140)(70)=437{,}000\ \text{mm}^3$$
$$\tau_{max}=\frac{VQ}{It_w}=\frac{35{,}000(437{,}000)}{111.6\times10^6(15)}
=\boxed{9.14\ \text{MPa}}\quad(<60\ \text{MPa allowable, OK})$$
Part (b): shear stress at point E. Point E sits at the very outer tip
(free edge) of the bottom flange — the first moment of area "beyond" that point, in the
direction shear flow would need to develop, is $Q=0$ (there is no material further out to
transfer force to). A free surface cannot sustain a complementary shear stress, so
$$\boxed{\tau_E = 0}$$
Shear stress in a thin-walled open section always falls to zero at every unconnected free edge;
it only builds up moving inward along the flange (feeding the shear flow into the web).