Question 2 of 6: Question 2 (paper Question II) — Forces in All Members of a Truss (Part A · Statics, equal value)
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Examination 04-BS-3, Statics and Dynamics — 2017-May. Candidates were required to answer any 2 of 3 questions in Part A (Statics) and any 2 of 3 in Part B (Dynamics); every question is solved below so this paper serves as a complete study resource (Questions 1–3 = paper Part A, I–III; Questions 4–6 = paper Part B, IV–VI).
Check — figure reconstruction. Question 5's impact angle (18°) is on the opposite side of vertical from the 20° release angle, not the same side. Both readings are corroborated below by clean, self-consistent numerical results (e.g. member D–F resolves to an exact 2.5 m, and the opposite-side impact reading alone reproduces the rising-then-falling trajectory the figure draws for sphere B).
Question 2 (paper Question II) — Forces in All Members of a Truss (Part A · Statics, equal value)
Given. A planar truss with joints A, B, C, D, E, F pinned at A (fixed/pin support) and B (roller support). Reading the figure gives the joint coordinates below and nine members: AB, AC, AD, BD, CD, CE, DE, DF, EF. A 50 kN load acts at F, 60° below the horizontal, directed down and to the right.
Given data — joint coordinates (m), taken with A at the origin
Joint
x (m)
y (m)
Support / load
A
0
0
pin
B
1.0
−2.5
roller (vertical reaction)
C
1.0
1.0
—
D
2.0
0
—
E
2.5
1.5
—
F
4.0
1.5
50 kN @ 60° below horizontal
Find. The axial force (tension or compression) in every member.
Figure 2. Nine-member truss, pin at A, roller at B, 50 kN load at F.
Approach. Confirm static determinacy, find the two support reactions from global equilibrium, then solve the sixteen scalar joint-equilibrium equations ($\sum F_x=0,\ \sum F_y=0$ at each of the six joints) simultaneously for the nine member forces and three reactions (method of joints, matrix form) — equivalent to, but more reliable than, working joint-by-joint by hand through C, E, D, B.
Determinacy check. $m=9$ members, $r=3$ reaction components (2 at the pin A, 1 at the roller B), $j=6$ joints: $m+r=12=2j=12$ — statically determinate.
Resolve the applied load. $F_x=50\cos60^\circ=25.0\ \text{kN}$, $F_y=-50\sin60^\circ=-43.30\ \text{kN}$ at F.
Support reactions (global equilibrium). Taking moments about A ($\sum M_A=0$) with only $B_y$ (roller, 1.0 m to the right of A) and the load at F contributing: $$B_y(1.0)+\big[(4.0)(-43.30)-(1.5)(25.0)\big]=0\ \Rightarrow\ B_y=210.7\ \text{kN (up)}$$ Then $\sum F_x=0\Rightarrow A_x=-25.0\ \text{kN}$ (i.e. 25.0 kN pointing left) and $\sum F_y=0\Rightarrow A_y=-(B_y+F_y)=-167.4\ \text{kN}$ (i.e. 167.4 kN downward).
Method of joints (representative joint F). Only members EF (horizontal) and DF (along $(2.0,-1.5)/2.5$) meet the load at F: $$\sum F_y=0:\ T_{DF}\!\left(\dfrac{-1.5}{2.5}\right)+F_y=0\ \Rightarrow\ T_{DF}=-72.17\ \text{kN (compression)}$$ $$\sum F_x=0:\ T_{EF}+T_{DF}\!\left(\dfrac{2.0}{2.5}\right)+F_x=0\ \Rightarrow\ T_{EF}=82.74\ \text{kN (tension)}$$ Proceeding the same way through joints E, C, D and B (each now a 2-equation, 2-unknown system) and solving simultaneously with the reactions above gives the complete member set in the results table; every value below satisfies both joint equilibrium at all six joints and the global checks $\sum F_x=\sum F_y=\sum M_A=0$ to within rounding.
Final results — Question 2 (T = tension, C = compression)