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Slope deflection: continuous beam, I = 4x10^7 mm^4

Short answer

Using slope-deflection, fixed-end moments and equilibrium yield the end moments: M_AB = -0.32 kNm, M_BA = -0.63, M_BC = 0.63, M_CB = 43.17, M_CD = -43.17, M_DC = 31.75 kNm. The bending moment diagram shows these values with max sagging 40.63 kNm at 2 m in CD.

Analyze the continuous beam shown in figure below by the slope deflection method. Given I=4×107 mm4I = 4\times10^{7}\ \text{mm}^4 and E=200 kN/mm2E = 200\ \text{kN/mm}^2. Draw Bending Moment diagram. [Figure: beam ABCD, A and D fixed; AB = 4 m (EI); BC = 4 m (2EI) with 10 kN/m UDL; CD = 6 m (EI) with a 60 kN point load at the 2 m mark.]

Data: EI=200 kN/mm2×4×107 mm4=8×103EI=200\ \text{kN/mm}^2\times4\times10^7\ \text{mm}^4=8\times10^{3} kNm². Relative stiffness: AB = EI, BC = 2EI, CD = EI. A and D fixed. AB = 4 m (no load), BC = 4 m with 10 kN/m, CD = 6 m with 60 kN at 2 m from C. No settlement, so the moments do not depend on the numerical value of EI.

Fixed-end moments (clockwise +)

  • BC: ∓10×4212=∓13.33\mp\dfrac{10\times4^2}{12}=\mp13.33 kNm
  • CD (a=2a=2, b=4b=4): FEMCD=−60×2×4262=−53.33FEM_{CD}=-\dfrac{60\times2\times4^2}{6^2}=-53.33, FEMDC=+60×22×462=26.67FEM_{DC}=+\dfrac{60\times2^2\times4}{6^2}=26.67 kNm

Slope-deflection equations (θA=θD=0\theta_A=\theta_D=0)

  • MAB=2EI4(θB)M_{AB}=\frac{2EI}{4}\left(\theta_{B}\right)
  • MBA=2EI4(2θB)M_{BA}=\frac{2EI}{4}\left(2\theta_{B}\right)
  • MBC=2(2EI)4(2θB+θC)−13.33M_{BC}=\frac{2(2EI)}{4}\left(2\theta_{B} + \theta_{C}\right) - 13.33
  • MCB=2(2EI)4(2θC+θB)+13.33M_{CB}=\frac{2(2EI)}{4}\left(2\theta_{C} + \theta_{B}\right) + 13.33
  • MCD=2EI6(2θC)−53.33M_{CD}=\frac{2EI}{6}\left(2\theta_{C}\right) - 53.33
  • MDC=2EI6(θC)+26.67M_{DC}=\frac{2EI}{6}\left(\theta_{C}\right) + 26.67

Joint equilibrium

  • Joint B: MBA+MBC=0M_{BA}+M_{BC}=0
  • Joint C: MCB+MCD=0M_{CB}+M_{CD}=0
EI[3.00001.00001.00002.6667]{θBθC}={13.33340.000}EI\begin{bmatrix}3.0000 & 1.0000 \\ 1.0000 & 2.6667\end{bmatrix}\begin{Bmatrix}\theta_{B} \\ \theta_{C}\end{Bmatrix}=\begin{Bmatrix}13.333 \\ 40.000\end{Bmatrix} EIθB=−0.6349,EIθC=15.2381EI\theta_{B}=-0.6349,\quad EI\theta_{C}=15.2381

With EI=8000EI=8000 kNm²: θB=−0.000079\theta_B=-0.000079 rad and θC=0.001905\theta_C=0.001905 rad (clockwise positive).

Final end moments (kNm)

EndMM (kNm)EndMM (kNm)
AB-0.32BA-0.63
BC0.63CB43.17
CD-43.17DC31.75

Checks:

  • Joint B: (-0.63) + (0.63) = 0.00 kNm (applied clockwise moment 0.00) ✓
  • Joint C: (43.17) + (-43.17) = 0.00 kNm (applied clockwise moment 0.00) ✓

Bending moment diagram ordinates (sagging +, kNm)

MemberBM at first endBM at second endMax within member
AB-0.320.63-
BC0.63-43.174.73 at 0.91 m
CD-43.17-31.7540.63 at 2.00 m

Reactions: A: H=0.00H=0.00, V=0.24V=0.24, M=0.32M=0.32; B: H=0.00H=0.00, V=8.81V=8.81, M=0.00M=0.00; C: H=0.00H=0.00, V=72.86V=72.86, M=0.00M=0.00; D: H=0.00H=0.00, V=18.10V=18.10, M=−31.75M=-31.75.

Answer: MAB=−0.32M_{AB}=-0.32, MBA=−0.63M_{BA}=-0.63, MBC=0.63M_{BC}=0.63, MCB=43.17M_{CB}=43.17, MCD=−43.17M_{CD}=-43.17, MDC=31.75M_{DC}=31.75 kNm (clockwise end moments +).

✓ Answer checked by Claude Opus 5.5 (high effort)

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