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Slope deflection: B sinks, C rises

Short answer

Applying the slope-deflection method with chord rotations due to support settlements (B sinks 10 mm, C rises 20 mm), the equilibrium equations give the end moments: M_AB=-112.13 kNm, M_BA=-116.26 kNm, M_BC=116.26 kNm, M_CB=138.02 kNm, M_CD=-138.02 kNm, M_DC=-119.01 kNm.

A continuous beam is shown in figure, support 'B' sinks by 10 mm down and 'C' rises by 20 mm up during loads. Analyse the given beam using the slope deflection method and also draw bending moment diagram and show deflected shape. E=200×106 kN/m2E = 200\times10^{6}\ \text{kN/m}^2 and I=80×10−6 m4I = 80\times10^{-6}\ \text{m}^4. [Figure: beam ABCD, A and D fixed; 12 kN in AB (1.5EI), 10 kN in BC (2EI), 5 kN/m UDL on CD (EI); dimensions 4 m, 2 m, 3 m, 3 m, 4 m as marked (exact load positions unclear).]

Data and assumptions: EI=200×106×80×10−6=16 000EI=200\times10^6\times80\times10^{-6}=16\,000 kNm². AB = 4 m (1.5EI) with 12 kN at mid-span; BC = 6 m (2EI) with 10 kN at mid-span; CD = 4 m (EI) with 5 kN/m; A and D are fixed. B sinks 10 mm, C rises 20 mm.

Chord rotations (clockwise +)

  • ψAB=0.0104=0.00250\psi_{AB}=\dfrac{0.010}{4}=0.00250 (B goes down)
  • ψBC=−(0.020+0.010)6=−0.00500\psi_{BC}=\dfrac{-(0.020+0.010)}{6}=-0.00500 (C is 30 mm higher than B, so the chord turns anticlockwise)
  • ψCD=0.0204=0.00500\psi_{CD}=\dfrac{0.020}{4}=0.00500 (D is 20 mm lower than C)

Fixed-end moments (kNm, clockwise +)

  • AB: ∓12×48=∓6\mp\dfrac{12\times4}{8}=\mp6
  • BC: ∓10×68=∓7.5\mp\dfrac{10\times6}{8}=\mp7.5
  • CD: ∓5×4212=∓6.67\mp\dfrac{5\times4^2}{12}=\mp6.67

Slope-deflection equations

  • MAB=12000.00(θB)−96.00M_{AB}=12000.00\left(\theta_{B}\right) - 96.00
  • MBA=12000.00(2θB)−84.00M_{BA}=12000.00\left(2\theta_{B}\right) - 84.00
  • MBC=10666.67(2θB+θC)+152.50M_{BC}=10666.67\left(2\theta_{B} + \theta_{C}\right) + 152.50
  • MCB=10666.67(2θC+θB)+167.50M_{CB}=10666.67\left(2\theta_{C} + \theta_{B}\right) + 167.50
  • MCD=8000.00(2θC)−126.67M_{CD}=8000.00\left(2\theta_{C}\right) - 126.67
  • MDC=8000.00(θC)−113.33M_{DC}=8000.00\left(\theta_{C}\right) - 113.33

Equilibrium and solution

MBA+MBC=0M_{BA}+M_{BC}=0 and MCB+MCD=0M_{CB}+M_{CD}=0:

[45333.333310666.666710666.666737333.3333]{θBθC}={−68.500−40.833}\begin{bmatrix}45333.3333 & 10666.6667 \\ 10666.6667 & 37333.3333\end{bmatrix}\begin{Bmatrix}\theta_{B} \\ \theta_{C}\end{Bmatrix}=\begin{Bmatrix}-68.500 \\ -40.833\end{Bmatrix} θB=−0.00134403,θC=−0.000709741\theta_{B}=-0.00134403,\quad \theta_{C}=-0.000709741

Final end moments (kNm)

EndMM (kNm)EndMM (kNm)
AB-112.13BA-116.26
BC116.26CB138.02
CD-138.02DC-119.01

Checks:

  • Joint B: (-116.26) + (116.26) = 0.00 kNm (applied clockwise moment 0.00) ✓
  • Joint C: (138.02) + (-138.02) = 0.00 kNm (applied clockwise moment 0.00) ✓

Bending moment diagram ordinates (sagging +, kNm)

MemberBM at first endBM at second endMax within member
AB-112.13116.26-
BC116.26-138.02-
CD-138.02119.01-

Deflected shape

  • A and D: fixed (zero deflection, zero slope).
  • B: moves down 10 mm; rotation θB=−0.00134\theta_B=-0.00134 rad (clockwise +).
  • C: moves up 20 mm; rotation θC=−0.00071\theta_C=-0.00071 rad.
  • The curve is concave upward (sagging) where the BM is positive and concave downward (hogging) where it is negative; the points of contraflexure (BM = 0) are at: AB at 1.78 m from its first end, BC at 3.09 m from its first end, CD at 1.99 m from its first end.
  • The curve falls from A to B, rises across BC from the low point at B to the raised support C, and then falls again to the fixed end D. At every fixed end the tangent is horizontal.

Reactions (kN, kNm): A: H=0.00H=0.00, V=63.10V=63.10, M=112.13M=112.13; B: H=0.00H=0.00, V=−88.48V=-88.48, M=0.00M=0.00; C: H=0.00H=0.00, V=121.64V=121.64, M=0.00M=0.00; D: H=0.00H=0.00, V=−54.26V=-54.26, M=119.01M=119.01.

Answer: MAB=−112.13M_{AB}=-112.13, MBA=−116.26M_{BA}=-116.26, MBC=116.26M_{BC}=116.26, MCB=138.02M_{CB}=138.02, MCD=−138.02M_{CD}=-138.02, MDC=−119.01M_{DC}=-119.01 kNm.

✓ Answer checked by Claude Opus 5.5 (high effort)

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