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Stiffness method: final end moments, frame

Short answer

Using stiffness method with unknowns θ_B, θ_C, θ_E (hinge at E). Slope-deflection equations, equilibrium at joints B, C and M_EB=0 give a 3×3 matrix. Solution: EIθ_B=4.79, EIθ_C=-9.44, EIθ_E=2.61. Final moments (kNm): M_AB=7.18, M_BA=14.37, M_BC=-16.55, M_CB=5.39, M_BE=22.18, M_EB=0, M_CD=-5.39, M_DC=-2.70.

Compute the final end moments for the following loaded frame using the stiffness method. [Figure: frame with A fixed at the left end of beam AB (3EI, 4 m); 20 kNm moment at B; beam BC (2EI, 5 m) with 8 kN/m UDL; column BE (2EI) with 20 kN horizontal load, E hinged at the base; column CD (EI) of height 7 m, D fixed; dimensions 4 m, 5 m as marked.]

Assumptions (figure partly unclear): A(0,0), B(4,0), C(9,0) lie on one horizontal girder: AB = 4 m (3EI), BC = 5 m (2EI) with 8 kN/m downward. Column BE (2EI) is 4 m long and carries the 20 kN horizontal load (to the right) at its mid-height; E is a hinge. Column CD (EI) is 7 m long and fixed at D. A is fixed. The 20 kNm moment at B is clockwise. Because A is fixed, the girder cannot sway, so the unknowns are only the joint rotations θB,θC\theta_B,\theta_C and the hinge rotation θE\theta_E.

Fixed-end moments (clockwise +)

  • BC: ∓wL212=∓8×5212=∓16.67\mp\dfrac{wL^2}{12}=\mp\dfrac{8\times5^2}{12}=\mp16.67 kNm
  • BE (point load 20 kN at mid-height): ∓PL8=∓20×48=∓10\mp\dfrac{PL}{8}=\mp\dfrac{20\times4}{8}=\mp10 kNm (for the load acting to the right on this downward member: FEMBE=10.00FEM_{BE}=10.00, FEMEB=−10.00FEM_{EB}=-10.00 kNm)
  • AB and CD: no loads, so zero.

Slope-deflection (stiffness) equations

  • MAB=2(3EI)4(θB)M_{AB}=\frac{2(3EI)}{4}\left(\theta_{B}\right)
  • MBA=2(3EI)4(2θB)M_{BA}=\frac{2(3EI)}{4}\left(2\theta_{B}\right)
  • MBC=2(2EI)5(2θB+θC)−16.67M_{BC}=\frac{2(2EI)}{5}\left(2\theta_{B} + \theta_{C}\right) - 16.67
  • MCB=2(2EI)5(2θC+θB)+16.67M_{CB}=\frac{2(2EI)}{5}\left(2\theta_{C} + \theta_{B}\right) + 16.67
  • MBE=2(2EI)4(2θB+θE)+10.00M_{BE}=\frac{2(2EI)}{4}\left(2\theta_{B} + \theta_{E}\right) + 10.00
  • MEB=2(2EI)4(2θE+θB)−10.00M_{EB}=\frac{2(2EI)}{4}\left(2\theta_{E} + \theta_{B}\right) - 10.00
  • MCD=2EI7(2θC)M_{CD}=\frac{2EI}{7}\left(2\theta_{C}\right)
  • MDC=2EI7(θC)M_{DC}=\frac{2EI}{7}\left(\theta_{C}\right)

Equilibrium

  • Joint B: MBA+MBC+MBE=20M_{BA}+M_{BC}+M_{BE}=20 (applied clockwise moment)
  • Joint C: MCB+MCD=0M_{CB}+M_{CD}=0
  • Hinge E: MEB=0M_{EB}=0
EI[6.60000.80001.00000.80002.17140.00001.00000.00002.0000]{θBθCθE}={26.667−16.66710.000}EI\begin{bmatrix}6.6000 & 0.8000 & 1.0000 \\ 0.8000 & 2.1714 & 0.0000 \\ 1.0000 & 0.0000 & 2.0000\end{bmatrix}\begin{Bmatrix}\theta_{B} \\ \theta_{C} \\ \theta_{E}\end{Bmatrix}=\begin{Bmatrix}26.667 \\ -16.667 \\ 10.000\end{Bmatrix} EIθB=4.7900,EIθC=−9.4402,EIθE=2.6050EI\theta_{B}=4.7900,\quad EI\theta_{C}=-9.4402,\quad EI\theta_{E}=2.6050

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

EndMM (kNm)EndMM (kNm)
AB7.18BA14.37
BC-16.55CB5.39
BE22.18EB0.00
CD-5.39DC-2.70

Checks:

  • Joint B: (14.37) + (-16.55) + (22.18) = 20.00 kNm (applied clockwise moment 20.00) ✓
  • Joint C: (5.39) + (-5.39) = 0.00 kNm (applied clockwise moment 0.00) ✓
  • Joint E: (0.00) = 0.00 kNm (applied clockwise moment 0.00) ✓
  • Hinge: MEB=0.00M_{EB}=0.00 ✓

Bending moment ordinates (sagging/inside + according to member direction):

MemberBM at first endBM at second endMax within member
AB7.18-14.37-
BC-16.55-5.3914.34 at 2.78 m
BE22.180.00-8.91 at 2.00 m
CD-5.392.70-

Reactions: A: H=−14.39H=-14.39, V=−5.39V=-5.39, M=−7.18M=-7.18; E: H=−4.45H=-4.45, V=27.62V=27.62, M=0.00M=0.00; D: H=−1.16H=-1.16, V=17.77V=17.77, M=2.70M=2.70.

Answer: MAB=7.18M_{AB}=7.18, MBA=14.37M_{BA}=14.37, MBC=−16.55M_{BC}=-16.55, MCB=5.39M_{CB}=5.39, MBE=22.18M_{BE}=22.18, MEB=0M_{EB}=0, MCD=−5.39M_{CD}=-5.39, MDC=−2.70M_{DC}=-2.70 kNm.

✓ Answer checked by Claude Opus 5.5 (high effort)

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