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16-Civ-A1 Elementary Structural Analysis · December 2016

Question 6 of 8: Two-pinned portal frame — reactions and diagrams

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

Notes on this paper

Reference texts: R.C. Hibbeler, Structural Analysis (10th ed., Pearson) — determinacy (Ch. 2), method of joints/sections (Ch. 3), shear & moment diagrams (Ch. 4), virtual-work deflections (Ch. 8–9), influence lines (Ch. 6), moment distribution / slope–deflection (Ch. 11–12); A. Kassimali, Structural Analysis (6th ed., Cengage) — internal hinges, compound (Gerber) beams, three-hinged and two-hinged frames. Sign convention: sagging bending moment positive; upward reactions positive; member tension positive (T), compression negative (C).

The paper directs candidates to answer Q1–Q5 and then one of Q6/Q7/Q8. For completeness all eight questions are worked here. Because every structure is defined entirely by its figure, each drawing has been read from the printed figure and redrawn to scale below.

Question 6: Two-pinned portal frame — reactions and diagrams (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. Symmetric portal: pin at (1)$=(0,0)$ and (4)$=(13,0)$; corners (2)$=(3,4)$, (3)$=(10,4)$; $13\text{ kN/m}$ UDL on the $7\text{ m}$ top beam (2)–(3); inclined legs rise $4$ m over $3$ m. Uniform $EI$.

Find. Reactions and the $V,M$ diagrams for members (2)–(3) and (3)–(4).

13 kN/m3 m7 m3 m4 m(1)(2)(3)(4)
Q6 — symmetric two-hinged portal (indeterminate to 1°).

Approach. With two pinned bases the frame is indeterminate to the 1st degree; the horizontal thrust $H$ is the redundant. By symmetry the vertical reactions are equal. For a uniform-$EI$ two-pinned frame $H$ follows from $\displaystyle H=\frac{\int M_0\,m_1/EI\,ds}{\int m_1^2/EI\,ds}$ — $EI$ cancels, which is why the problem needs no numerical $EI$.

  1. Vertical reactions. Total load $=13(7)=91\text{ kN}$; by symmetry $R_{(1)}=R_{(4)}=\boxed{45.5\text{ kN}\uparrow}$.
  2. Horizontal thrust. Releasing one horizontal reaction and enforcing zero relative horizontal displacement gives $H=\boxed{43.1\text{ kN}}$ (inward at each base).
  3. Corner moments. $M_{(2)}=M_{(3)}=\boxed{-35.96\text{ kN}\cdot\text{m}}$ (hogging).
  4. Member (2)–(3). With hogging ends $-35.96$ and free sagging $\tfrac{13(7)^2}{8}=79.6$, the mid-span moment is $-35.96+79.6=\boxed{+43.66\text{ kN}\cdot\text{m}}$ (sagging). Shear runs $+45.5$ at (2) to $-45.5$ at (3), zero at mid-span.
  5. Member (3)–(4). The unloaded leg carries a straight-line moment from $\boxed{-35.96\text{ kN}\cdot\text{m}}$ at (3) to $0$ at the pin (4); axial compression $\approx62.3\text{ kN}$, constant shear $\approx7.2\text{ kN}$.
BMD member ②–③ (kN·m)−36−36+43.7BMD member ③–④ (kN·m) — leg−36 (node ③)0 (node ④)
Q6 — moment diagrams of the loaded beam (2)–(3) and the leg (3)–(4).