Skip to main content

Truss: rectangular, diagonal 2 cm too short

Short answer

Take H_B as redundant; compatibility includes BD lack-of-fit 20 mm. Final forces (kN): BC=-85.33, CD=-113.77, DA=-10.33, AC=142.21, BD=17.21 (+ tension, – compression); AB zero.

A rectangular horizontal truss of span 12 m and height 9 m is with two diagonals and is supported by two hinges fixed at the base. A horizontal force of magnitude 100 kN is acting toward the truss at the left top joint. The diagonal connecting the loaded joint was manufactured 2 cm shorter than the assigned length. Calculate the forces induced in every member assuming Young's modulus and cross-sectional areas of every member to be 2×1052\times10^{5} MPa and 1000 mm² respectively.

Setup: joints A(0,0) and B(12,0) at the base (both hinges), C(12,9) and D(0,9) at the top. Members: verticals AD, BC; top chord CD; diagonals AC and BD (bottom chord AB is not a member between the two hinges, or if present it carries no force because A and B cannot move). 100 kN acts horizontally to the right at D (the loaded joint). The diagonal BD joining the loaded joint is 20 mm short. E=2×105E=2\times10^5 MPa, A=1000A=1000 mm², so EA=2×105EA=2\times10^5 kN and lengths: AD = BC = 9 m, CD = 12 m, AC = BD = 15 m.

Degree of indeterminacy

m=5m=5, r=4r=4, j=4j=4: Ds=5+4−8=1D_s=5+4-8=1. Take the horizontal reaction at B, X=HBX=H_B (to the right +), as the redundant. In the primary truss B is a roller on the base line.

Forces in the primary truss

S0S_0 = bar forces due to the 100 kN load (the lack of fit is treated separately). S1S_1 = bar forces due to a unit force at B acting to the right.

BarL (m)S0S_0 (kN)S1S_1S0S1LS_0S_1LS12LS_1^2LFinal SS (kN)
BC9.000-75.00-0.7500506.2505.0625-85.33
CD12.000-100.00-1.00001200.00012.0000-113.77
DA9.0000.00-0.75000.0005.0625-10.33
AC15.000125.001.25002343.75023.4375142.21
BD15.0000.001.25000.00023.437517.21
Sum4050.0069.000

Lack of fit term

The bar BD is shorter by 20 mm, i.e. its free elongation is e0=−0.02e_0=-0.02 m. It contributes S1e0=1.2500×(−0.02)=−0.02500S_1e_0=1.2500\times(-0.02)=-0.02500 m to the displacement at B.

Compatibility (HBH_B gives no horizontal movement at B)

∑S0S1LEA+∑S1e0+X∑S12LEA=0\frac{\sum S_0S_1L}{EA}+\sum S_1e_0+X\frac{\sum S_1^2L}{EA}=0 4050.0002×105+(−0.02500)+X69.00002×105=0  ⇒  X=HB=13.77 kN\frac{4050.000}{2\times10^5}+(-0.02500)+X\frac{69.0000}{2\times10^5}=0\;\Rightarrow\; X=H_B=13.77\ \text{kN}

(positive: HBH_B acts to the right, in the same direction as the 100 kN load.)

Bar forces (S=S0+XS1S=S_0+XS_1, + tension, - compression)

BC = -85.33, CD = -113.77, DA = -10.33, AC = 142.21, BD = 17.21 kN.

Reactions: HB=13.77H_B=13.77 kN (right), HA=−113.77H_A=-113.77 kN, i.e. 113.77 kN to the left; vertical reactions VA=−75.00V_A=-75.00 kN and VB=75.00V_B=75.00 kN (couple of the 100 kN load). The result was checked with a full stiffness analysis.

Answer: BC = -85.33, CD = -113.77, DA = -10.33, AC = 142.21, BD = 17.21 kN (+ tension, - compression); AB carries zero.

✓ Answer checked by Claude Opus 5.5 (high effort)

All Theory of Structures II chapter 2 questions →