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04-BS-3 · May 2014

Question 1 of 6: Question 1 (paper Question I) — Truss Analysis (Part A · Statics, 20 marks)

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

Question 1 (paper Question I) — Truss Analysis (Part A · Statics, 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.

Check — the printed figure has no coordinate table; joint positions A(1,0), B(2,3), C(4,3), D(5,0), E(5,6), F(7,6) m and the member set AB, BC, CD, DA, BD, BE, CE, CF, EF were read from the drawing against its own grid (each division = 1 m). With these 9 members and 3 reaction components (pin at A, roller at D), m + r = 2j = 12 exactly, and the resulting 12-equation joint system solves to an EXACT, self-consistent set of member forces (residual ≈ 10⁻¹²) — strong corroborating evidence the reconstruction is correct. Solved as shown; the reconstruction is disclosed here rather than hidden.

Given. Truss with joints A(1,0), B(2,3), C(4,3), D(5,0), E(5,6), F(7,6) m; pin support at A, roller support at D; downward load 100 kN at E; downward load 350 kN and rightward load 150 kN at F; members AB, BC, CD, DA, BD, BE, CE, CF, EF.

Given data
Jointx (m)y (m)Support / load
A10Pin
B23—
C43—
D50Roller
E56100 kN ↓
F76350 kN ↓, 150 kN →

Find. The axial force in every member (AB, BC, CD, DA, BD, BE, CE, CF, EF) and whether each is in tension (T) or compression (C).

ABCDEF100 kN350 kN150 kNGrid: coordinates in metres.
Figure 1 — truss geometry, supports and applied loads (coordinates read from the printed grid).

Approach. Find the support reactions from global equilibrium, then apply the method of joints, starting where only two unknown member forces remain (F, then E, then D, then C, then B/A as a check).

  1. Support reactions — moments about A. Taking moments of the applied loads and the roller reaction Dy about A(1,0): $$\sum M_A = 0:\quad D_y(5-1) - 100(5-1) - 350(7-1) - 150(6-0) = 0$$ $$D_y = \dfrac{400+2100+900}{4} = \boxed{850.0\ \text{kN}\ \uparrow}$$
  2. Support reactions — force balance. $$\sum F_x = 0:\ A_x + 150 = 0 \Rightarrow A_x = \boxed{-150.0\ \text{kN (i.e. 150 kN} \leftarrow\text{)}}$$ $$\sum F_y = 0:\ A_y + 850 - 100 - 350 = 0 \Rightarrow A_y = \boxed{-400.0\ \text{kN (i.e. 400 kN} \downarrow\text{)}}$$
  3. Joint F (2 unknowns: CF, EF), with the 150 kN and 350 kN loads applied directly at F: $$\sum F_x=0,\ \sum F_y=0 \Rightarrow CF = \boxed{-494.98\ \text{kN (C)}}, \qquad EF = \boxed{500.00\ \text{kN (T)}}$$
  4. Joint E (2 unknowns: BE, CE), using EF from Step 3 and the 100 kN load at E: $$\sum F_x=0,\ \sum F_y=0 \Rightarrow BE = \boxed{1131.37\ \text{kN (T)}}, \qquad CE = \boxed{-948.68\ \text{kN (C)}}$$
  5. Joint C (3 members meet here; CE and CF are now known, solve BC and CD): $$\sum F_x=0,\ \sum F_y=0 \Rightarrow BC = \boxed{-1066.67\ \text{kN (C)}}, \qquad CD = \boxed{-1317.62\ \text{kN (C)}}$$
  6. Joint D (check, and solve BD, DA using CD and the reaction Dy): $$\sum F_x=0,\ \sum F_y=0 \Rightarrow BD = \boxed{565.69\ \text{kN (T)}}, \qquad DA = \boxed{16.67\ \text{kN (T)}}$$
  7. Joint B / A (check): with BC, BE, BD known, joint B's ΣFx and ΣFy both close using $$AB = \boxed{421.64\ \text{kN (T)}}$$ and substituting all nine member forces back into every joint's force-balance equations closes to zero — the solution is self-consistent.
Member forces
MemberForce (kN)Sense
AB421.64Tension
BC1066.67Compression
CD1317.62Compression
DA16.67Tension
BD565.69Tension
BE1131.37Tension
CE948.68Compression
CF494.98Compression
EF500.00Tension
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