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Truss: lack of fit, temperature, bars BC BF

Short answer

Take the B roller reaction as redundant and impose zero displacement at B. Compatibility gives X=179.80 kN, so BC=0.00 kN and BF=-174.73 kN compression.

Determine forces in bars BC and BF of the truss shown below, if all inclined members are found to be 2 mm too long and all vertical members are subjected to a decrease in temperature of 15°C. Area of cross-section of all members is 40 cm². Take E=2×105 N/mm2E = 2\times10^{5}\ \text{N/mm}^2, α=10.8×10−6/°C\alpha = 10.8\times10^{-6}/°C. [Figure: truss with joints A, B, C on the bottom chord (A hinged, B roller, C roller; 5 m + 5 m), D, E, F on the top chord, height 3 m, with vertical and inclined members.]

Assumptions (figure read as follows): bottom joints A(0,0), B(5,0), C(10,0); top joints D(0,3), E(5,3), F(10,3). Members: bottom chord AB, BC; top chord DE, EF; verticals AD, BE, CF; inclined members DB and BF. A is a hinge; B and C are rollers (vertical reactions only). All areas 40 cm², E=2×105E=2\times10^5 N/mm², so EA=8×105EA=8\times10^5 kN. The inclined members DB and BF are 2 mm too long; the verticals AD, BE, CF are cooled by 15°C (α=10.8×10−6\alpha=10.8\times10^{-6}/°C).

Degree of indeterminacy

m=9m=9, r=4r=4, j=6j=6: Ds=9+4−12=1D_s=9+4-12=1. The truss is internally determinate, so the lack of fit and the temperature change only produce forces because of the extra support. Take the vertical reaction at B as the redundant XX.

Free (initial) elongations e0e_0

  • Inclined bars too long: e0=+2e_0=+2 mm (DB and BF).
  • Verticals cooled: e0=−α ΔT L=−10.8×10−6×15×3000=−0.486e_0=-\alpha\,\Delta T\,L=-10.8\times10^{-6}\times15\times3000=-0.486 mm.

Unit load on the primary truss

The primary truss (B roller removed) is loaded by a unit upward force at B, giving S1S_1. Since no external load acts, S0=0S_0=0 and only the initial strains cause displacement of B.

BarL (m)S1S_1e0e_0 (mm)S1e0S_1e_0 (mm)S12LS_1^2L (m)Final SS (kN)
AB5.0000.0000.0000.00000.0000.00
BC5.0000.0000.0000.00000.0000.00
DE5.0000.8330.0000.00003.472149.83
EF5.0000.8330.0000.00003.472149.83
AD3.0000.500-0.486-0.24300.75089.90
BE3.0000.000-0.4860.00000.0000.00
CF3.0000.500-0.486-0.24300.75089.90
DB5.831-0.9722.000-1.94375.507-174.73
BF5.831-0.9722.000-1.94375.507-174.73
ΔB=∑S1e0=−3.8873+(−0.4860)=−4.3733 mm(negative: B moves 4.373 mm downward in the primary truss)\Delta_{B}=\sum S_1e_0=-3.8873+(-0.4860)=-4.3733\ \text{mm}\quad(\text{negative: B moves 4.373 mm downward in the primary truss}) f11=∑S12LEA=19.4588×105=0.02432 mm/kNf_{11}=\frac{\sum S_1^2L}{EA}=\frac{19.458}{8\times10^5}=0.02432\ \text{mm/kN}

Compatibility (BB cannot move): ΔB+f11X=0\Delta_B+f_{11}X=0

X=−−4.37330.02432=179.80 kNX=-\frac{-4.3733}{0.02432}=179.80\ \text{kN}

Bar forces S=XS1S=XS_1 (S0=0S_0=0, because the initial strains alone produce no forces in the statically determinate primary truss):

Answer: force in BC = 0.00 kN and force in BF = -174.73 kN (+ tension, - compression). Other bars: AB = 0.00, DE = 149.83, EF = 149.83, AD = 89.90, BE = 0.00, CF = 89.90, DB = -174.73 kN.

✓ Answer checked by Claude Opus 5.5 (high effort)

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