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Slope deflection: beam with settlement of C

Short answer

Using slope-deflection with chord rotations from 4 mm settlement, fixed-end moments are computed and joint equilibrium equations solved. Final end moments: M_AB=0, M_BA=3.21, M_BC=-3.21, M_CB=0.27, M_CD=-0.27, M_DC=3.90 tm.

Analyse the continuous beam loaded as shown in figure below using the slope deflection method considering settlement of support C by 4 mm downward. Take EI=1×109 t mm2EI = 1\times10^{9}\ \text{t mm}^2. [Figure: continuous beam ABCD, D fixed; 2 t point load near A; 3 t/m UDL on BC (3I); 5 t point load on CD (I); dimensions 2 m, 1.5 m, 2 m, 4 m, 3 m and 1 m as marked.]

Assumptions (dimensions are not fully legible): A is a pin (free to rotate), AB = 3.5 m with the 2 t load 2 m from A; BC = 4 m (3I) with 3 t/m; CD = 4 m (I) with the 5 t load 3 m from C (1 m from D); D is fixed; B and C are simple supports. Units: tonne, metre. EI=1×109 t mm2=1000EI=1\times10^9\ \text{t mm}^2=1000 t m². Support C settles δ=4\delta=4 mm = 0.004 m.

Chord rotations (clockwise +, a member whose right end sinks rotates clockwise)

ψBC=0.0044=0.0010\psi_{BC}=\dfrac{0.004}{4}=0.0010 (C goes down relative to B), ψCD=−0.0044=−0.0010\psi_{CD}=-\dfrac{0.004}{4}=-0.0010 (D is higher than C). ψAB=0\psi_{AB}=0.

Fixed-end moments (tm, clockwise +)

  • AB: FEMAB=−2×2×1.523.52=−0.735FEM_{AB}=-\dfrac{2\times2\times1.5^2}{3.5^2}=-0.735, FEMBA=+2×22×1.53.52=0.980FEM_{BA}=+\dfrac{2\times2^2\times1.5}{3.5^2}=0.980
  • BC: ∓3×4212=∓4.000\mp\dfrac{3\times4^2}{12}=\mp4.000
  • CD: FEMCD=−5×3×1242=−0.938FEM_{CD}=-\dfrac{5\times3\times1^2}{4^2}=-0.938, FEMDC=+5×32×142=2.812FEM_{DC}=+\dfrac{5\times3^2\times1}{4^2}=2.812

Slope-deflection equations (Mij=2EIL(2θi+θj−3ψ)+FEMijM_{ij}=\tfrac{2EI}{L}(2\theta_i+\theta_j-3\psi)+FEM_{ij}, numerical)

  • MAB=571.43(2θA+θB)−0.73M_{AB}=571.43\left(2\theta_{A} + \theta_{B}\right) - 0.73
  • MBA=571.43(2θB+θA)+0.98M_{BA}=571.43\left(2\theta_{B} + \theta_{A}\right) + 0.98
  • MBC=1500.00(2θB+θC)−8.50M_{BC}=1500.00\left(2\theta_{B} + \theta_{C}\right) - 8.50
  • MCB=1500.00(2θC+θB)−0.50M_{CB}=1500.00\left(2\theta_{C} + \theta_{B}\right) - 0.50
  • MCD=500.00(2θC)+0.56M_{CD}=500.00\left(2\theta_{C}\right) + 0.56
  • MDC=500.00(θC)+4.31M_{DC}=500.00\left(\theta_{C}\right) + 4.31

Joint equilibrium

MAB=0M_{AB}=0; MBA+MBC=0M_{BA}+M_{BC}=0; MCB+MCD=0M_{CB}+M_{CD}=0 (θ in radians)

[1142.8571571.42860.0000571.42864142.85711500.00000.00001500.00004000.0000]{θAθBθC}={0.7357.520−0.062}\begin{bmatrix}1142.8571 & 571.4286 & 0.0000 \\ 571.4286 & 4142.8571 & 1500.0000 \\ 0.0000 & 1500.0000 & 4000.0000\end{bmatrix}\begin{Bmatrix}\theta_{A} \\ \theta_{B} \\ \theta_{C}\end{Bmatrix}=\begin{Bmatrix}0.735 \\ 7.520 \\ -0.062\end{Bmatrix} θA=−0.000446259,θB=0.00217823,θC=−0.000832462\theta_{A}=-0.000446259,\quad \theta_{B}=0.00217823,\quad \theta_{C}=-0.000832462

Final end moments (tm, clockwise on the member end +)

EndMM (tm)EndMM (tm)
AB0.00BA3.21
BC-3.21CB0.27
CD-0.27DC3.90

Checks:

  • Pin A: MAB=0.00M_{AB}=0.00 tm ✓
  • Joint B: (3.21) + (-3.21) = 0.00 tm ✓
  • Joint C: (0.27) + (-0.27) = 0.00 tm ✓

Bending moments (sagging +, tm)

MemberBM at first endBM at second endMax within member
AB0.00-3.21-0.12 at 2.00 m (under the 2 t load)
BC-3.21-0.274.35 at 2.25 m
CD-0.27-3.900.76 at 3.00 m

Reactions (t, tm): A: H=0.00H=0.00, V=−0.06V=-0.06, M=0.00M=0.00; B: H=0.00H=0.00, V=8.80V=8.80, M=0.00M=0.00; C: H=0.00H=0.00, V=5.61V=5.61, M=0.00M=0.00; D: H=0.00H=0.00, V=4.66V=4.66, M=−3.90M=-3.90.

Answer: MBA=3.214M_{BA}=3.214, MBC=−3.214M_{BC}=-3.214, MCB=0.270M_{CB}=0.270, MCD=−0.270M_{CD}=-0.270, MDC=3.896M_{DC}=3.896 tm; MAB=0M_{AB}=0.

✓ Answer checked by Claude Opus 5.5 (high effort)

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