Skip to main content

Truss: nodal displacements, reactions, member forces

Short answer

Direct stiffness solution gives u2=1.667 mm right and v2=3.958 mm up. Member forces are 166.67 kN tension in 1-2, 83.33 kN compression in 2-3, and zero in 1-3. Reactions are (-166.67, 0) kN at node 1 and (66.67, -50) kN at node 3.

Determine the nodal displacements, reaction forces and member forces of the given truss structure, loaded as shown in the figure. Given that for each member, sectional area A=2×10−3A = 2\times10^{-3} m2^2 and modulus of elasticity E=2×105E = 2\times10^5 MPa.

[Figure: three-member truss; node 1 at the origin (pinned), node 2 at 4 m to the right of node 1, node 3 at 3 m above node 1 (pinned); members 1-2, 2-3 and 1-3; at node 2 a 50 kN upward load and a 100 kN horizontal load (to the right)]

Data: node 1 (0,0)(0,0) pinned, node 2 (4,0)(4,0) loaded, node 3 (0,3)(0,3) pinned. A=2×10−3A=2\times10^{-3} m2^2, E=2×105E=2\times10^5 MPa =2×108=2\times10^8 kN/m2^2, so EA=4×105EA=4\times10^5 kN. Loads at node 2: Fx=100F_x=100 kN, Fy=50F_y=50 kN. Units: kN, m.

   3 (0,3)
   |\
   | \ 5 m
 3 m  \
   |   \    50 kN
   1----2 -> 100 kN
     4 m

Element data

Direction cosines c=xj−xiLc=\dfrac{x_j-x_i}{L}, s=yj−yiLs=\dfrac{y_j-y_i}{L}; axial stiffness EA/LEA/L.

MemberLL (m)ccssEA/LEA/L (kN/m)
1-241.00.0100000
2-35-0.80.680000
1-330.01.0133333

Element stiffness in global axes:

[k]=EAL[c2cs−c2−cscss2−cs−s2−c2−csc2cs−cs−s2css2][k]=\frac{EA}{L}\begin{bmatrix}c^2&cs&-c^2&-cs\\cs&s^2&-cs&-s^2\\-c^2&-cs&c^2&cs\\-cs&-s^2&cs&s^2\end{bmatrix}
  • Member 1-2: 105[10−100000−10100000]10^5\begin{bmatrix}1&0&-1&0\\0&0&0&0\\-1&0&1&0\\0&0&0&0\end{bmatrix} (DOFs u1,v1,u2,v2u_1,v_1,u_2,v_2)
  • Member 2-3: 104[5.12−3.84−5.123.84−3.842.883.84−2.88−5.123.845.12−3.843.84−2.88−3.842.88]10^4\begin{bmatrix}5.12&-3.84&-5.12&3.84\\-3.84&2.88&3.84&-2.88\\-5.12&3.84&5.12&-3.84\\3.84&-2.88&-3.84&2.88\end{bmatrix} (DOFs u2,v2,u3,v3u_2,v_2,u_3,v_3)
  • Member 1-3: 1.3333×1051.3333\times10^5 in the v1,v3v_1,v_3 terms only.

Assembly and solution

Nodes 1 and 3 are pinned (u1=v1=u3=v3=0u_1=v_1=u_3=v_3=0); free DOFs are u2,v2u_2,v_2. Adding the node-2 terms of members 1-2 and 2-3:

[151 200−38 400−38 40028 800]{u2v2}={10050}\begin{bmatrix}151\,200&-38\,400\\-38\,400&28\,800\end{bmatrix}\begin{Bmatrix}u_2\\v_2\end{Bmatrix}=\begin{Bmatrix}100\\50\end{Bmatrix} u2=1.6667 mm (→),v2=3.9583 mm (↑)u_2=1.6667\ \text{mm}\ (\rightarrow),\qquad v_2=3.9583\ \text{mm}\ (\uparrow)

Member forces

F=EAL [−c  −s  c  s]{d}F=\dfrac{EA}{L}\,[-c\ \ -s\ \ c\ \ s]\{d\}:

  • Member 1-2: 166.67166.67 kN (tension)
  • Member 2-3: −83.33-83.33 kN (compression)
  • Member 1-3: 0.000.00 kN (zero force, both ends fixed in the vertical direction)

Reactions {R}=[K]{d}−{F}\{R\}=[K]\{d\}-\{F\}

  • Node 1: Rx=−166.67R_x=-166.67 kN, Ry=0.00R_y=0.00 kN
  • Node 3: Rx=66.67R_x=66.67 kN, Ry=−50.00R_y=-50.00 kN

Check: ΣFx=−166.67+66.67+100=0\Sigma F_x=-166.67+66.67+100=0; ΣFy=0−50+50=0\Sigma F_y=0-50+50=0; ΣM1=50×4−66.67×3=0\Sigma M_1=50\times4-66.67\times3=0.

Answer: u2=1.667u_2=1.667 mm, v2=3.958v_2=3.958 mm; member forces 166.67 kN (T), 83.33 kN (C), 0; reactions (−166.67, 0)(-166.67,\,0) kN at node 1 and (66.67, −50)(66.67,\,-50) kN at node 3.

✓ Answer checked by Claude Opus 5.5 (high effort)

All Computational Techniques in Civil Engineering chapter 4 questions →