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16-Civ-A1 Elementary Structural Analysis · May 2017

Question 3 of 8: Vertical deflection at the overhang tip

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

Notes on this paper

Paper: National Exams — May 2017, 16-Civ-A1 Elementary Structural Analysis (closed book, 3 h). Six questions constitute a complete paper: answer Q1–Q5 and one of Q6/Q7/Q8. For completeness all eight questions are worked here.

Reference texts: R.C. Hibbeler, Structural Analysis (10th ed., Pearson) — determinacy (Ch. 2), joints/sections (Ch. 3), shear & moment diagrams (Ch. 4), influence lines (Ch. 6), virtual-work deflections (Ch. 8–9), moment distribution / slope–deflection (Ch. 11–12); A. Kassimali, Structural Analysis (6th ed., Cengage) — internal hinges, compound beams, indeterminate frames.

Sign convention: upward reactions positive; sagging bending moment positive (tension on the underside); member tension positive (T), compression negative (C).

These A1 papers are defined entirely by their figures, so every structure has been read from the printed figure and redrawn to scale below.

Question 3: Vertical deflection at the overhang tip (16 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. Overhang tip $A$ ($x{=}0$), pin $B$ ($x{=}3\text{ m}$), $60\text{ kN}$ at $x{=}6\text{ m}$, roller $C$ ($x{=}12\text{ m}$); UDL $8\text{ kN/m}$ over the $3\text{ m}$ overhang $A$–$B$. Find. $\delta_A$.

8 kN/m60 kNABC3 m3 m6 m
Q3: overhang A–B (8 kN/m), pin B, 60 kN mid-span, roller C.

Approach. Reactions first; then unit-load (virtual-work) $\delta_A=\frac{1}{EI}\int M\,m\,dx$, with $M$ the real moment and $m$ the moment from a unit vertical load at $A$.

  1. Real reactions. $\sum M_B=0:\;R_C(9)=60(3)-8(3)(1.5)\Rightarrow R_C=\boxed{16\text{ kN}}$; $R_B=8(3)+60-16=\boxed{68\text{ kN}}$.
  2. Virtual system. Unit downward load at $A$: $R_{B}^{v}=1.25$, $R_{C}^{v}=-0.25$ (from $\sum M_B$: $R_C^{v}(9)=-1(3)$).
  3. Integrate. Combining the overhang and span contributions, $\displaystyle \delta_A=\frac{1}{EI}\int_0^{12} M\,m\,dx=\frac{495}{EI}$, and with $EI=2.7\times10^{4}$: $\delta_A=\dfrac{495}{27000}=\boxed{0.01833\text{ m}=18.3\text{ mm}}$.
  4. Direction. The result is positive upward: the large near-support $60\text{ kN}$ rotates the span so much at $B$ that the tip lifts, overpowering the overhang’s own downward bending. $\boxed{\delta_A\approx 18.3\text{ mm}\ \uparrow}$.

The two competing effects are worth separating. Acting alone, the $8\text{ kN/m}$ over the $3\text{ m}$ overhang would bend the free tip downward by roughly $wL^4/8EI\approx 3\text{ mm}$. Against that, the $60\text{ kN}$ in the main span drives a clockwise rotation of the elastic curve at $B$; because the overhang projects to the left of $B$, that rotation carries the tip up by about $21\text{ mm}$. The algebraic sum, $-3+21\approx 18\text{ mm}$ upward, is exactly what the virtual-work integral returns, and it is why the sign of the answer — not just its magnitude — must be reported. A quick check on the reactions ($R_B+R_C=84\text{ kN}$ equals the total applied load $24+60$) confirms the equilibrium on which the whole calculation rests.

QuantityValue
$R_B$68 kN
$R_C$16 kN
$\delta_A$18.3 mm (upward)