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04-BS-6 · December 2016

Question 2 of 8: Deflection by Integration

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

National Exams December 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 wide-flange (W-shape) section-property table is attached at the end of the official exam; every question below supplies its own built-up section, so the table is not needed for any of the eight solutions.

Reference texts: Hibbeler, Mechanics of Materials, 10th ed. (shear/moment diagrams, deflection by integration, combined axial+bending, transformation of stress via Mohr's circle, torsion of stepped shafts, axial members and pin connections, Euler column buckling).

Question 2: Deflection by Integration (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. Same beam, loading and I-section as Question 1 (E = 200 GPa). The bending-moment expression $M(x)=120+10x-\tfrac{5}{6}x^{3}$ kN·m derived there carries over unchanged.

Find. The maximum deflection $y_{max}$, the slope $\theta_A$ at the left support, and whether $|y_{max}|$ clears the L/120 = 50 mm serviceability limit.

30 kN/m 120 kN·m 6 m A B 100 300 15 20 I-section (mm)
Loaded beam and I-section (unchanged from Question 1).

Approach. Integrate the Euler–Bernoulli equation $EI\,y''=M(x)$ twice; the two constants follow from the simply-supported boundary conditions $y(0)=y(L)=0$ (note this beam is pinned at BOTH ends, so neither slope is prescribed — only the deflections vanish).

  1. Section properties. For the 100×300 mm I-section (15 mm flanges, 20 mm web), $I=93.78\times10^{6}\ \text{mm}^4$, so $EI=18.76\times10^{12}\ \text{N}\!\cdot\!\text{mm}^2$.
  2. Integrate twice. With $M(x)$ in N·mm and $x$ in mm, $$EI\,y'=\int M(x)\,dx + C_1, \qquad EI\,y=\int\!\!\int M(x)\,dx\,dx + C_1x + C_2$$ Applying $y(0)=0$ gives $C_2=0$; applying $y(6000\text{ mm})=0$ then solves for $C_1$ (done symbolically, since the closed form is a lengthy quintic/quartic pair).
  3. Slope at A. Evaluating $y'(0)=C_1/EI$: $$\boxed{\theta_A=-0.01951\ \text{rad}=-1.1181^{\circ}}$$ (negative — the beam rotates downward-clockwise at A, as expected under a sagging deflection with the couple pinning $M(0^+)$ positive).
  4. Maximum deflection. Scanning $y(x)$ over the span (equivalently, solving $y'(x)=0$) locates the extremum at $x=2828$ mm: $$\boxed{y_{max}=-27.99\ \text{mm}}\quad(\text{downward})$$
  5. Serviceability check. The allowable limit is $L/120=6000/120=50.0$ mm. Since $|y_{max}|=27.99\ \text{mm} < 50.0\ \text{mm}$, the beam satisfies the deflection limit.
y_max = -27.99 mm (at x=2828 mm) allowable limit L/120 = 50.0 mm > |y_max| -> OK
Deflected shape (to a visually exaggerated vertical scale), with the location and magnitude of y_max marked.
QuantityValue
θA-1.9514e-02 rad (-1.1181°)
ymax-27.99 mm (downward), at x=2828 mm
Allowable L/12050.0 mm
CheckOK (28.0 mm < 50.0 mm)