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Stiffness matrix: final end moments, 2.5EI frame

Short answer

Stiffness method with unknowns theta_B, theta_C and sway Delta gives final moments M_AB=-3.78, M_BA=57.50, M_BC=-37.50, M_CB=65.57, M_CD=-65.57, M_DC=-48.14 kNm.

Compute the final end moments for the following loaded frame using the stiffness matrix method. [Figure: frame ABCD; beam BC (2EI) of 10 m with 8 kN/m UDL and 20 kNm moment at B; column AB (2.5EI) of height 6 m with 15 kN horizontal load 4 m above A, A fixed; column CD (2EI) of height 6 m, D fixed.]

Assumptions: A(0,0), B(0,6), C(10,6), D(10,0); the 20 kNm moment at B is clockwise; the 15 kN load acts to the right on AB at 4 m above A; the UDL of 8 kN/m acts downward on BC. A and D are fixed. Axial deformation is neglected.

Unknowns

θB,θC\theta_B,\theta_C and the sway Δ\Delta of the girder (right +); ψAB=ψCD=Δ/6\psi_{AB}=\psi_{CD}=\Delta/6.

Fixed-end moments

  • BC: ∓8×10212=∓66.67\mp\dfrac{8\times10^2}{12}=\mp66.67 kNm
  • AB (point load 15 kN at a = 4 m from A, b = 2 m): the load acts perpendicular to the member: FEMAB=−6.67FEM_{AB}=-6.67, FEMBA=13.33FEM_{BA}=13.33 kNm (from Pab2/L2Pab^2/L^2 and Pa2b/L2Pa^2b/L^2 with the sign for a load to the right)

Stiffness equations of the members

  • MAB=2(2.5EI)6(θB−(0.5000)Δ1)−6.67M_{AB}=\frac{2(2.5EI)}{6}\left(\theta_{B} - (0.5000)\Delta_1\right) - 6.67
  • MBA=2(2.5EI)6(2θB−(0.5000)Δ1)+13.33M_{BA}=\frac{2(2.5EI)}{6}\left(2\theta_{B} - (0.5000)\Delta_1\right) + 13.33
  • MBC=2(2EI)10(2θB+θC)−66.67M_{BC}=\frac{2(2EI)}{10}\left(2\theta_{B} + \theta_{C}\right) - 66.67
  • MCB=2(2EI)10(2θC+θB)+66.67M_{CB}=\frac{2(2EI)}{10}\left(2\theta_{C} + \theta_{B}\right) + 66.67
  • MCD=2(2EI)6(2θC−(0.5000)Δ1)M_{CD}=\frac{2(2EI)}{6}\left(2\theta_{C} - (0.5000)\Delta_1\right)
  • MDC=2(2EI)6(θC−(0.5000)Δ1)M_{DC}=\frac{2(2EI)}{6}\left(\theta_{C} - (0.5000)\Delta_1\right)

Equilibrium

  • Joint B: MBA+MBC=20M_{BA}+M_{BC}=20 (applied clockwise moment)
  • Joint C: MCB+MCD=0M_{CB}+M_{CD}=0
  • Storey shear: taking moments about B for column AB (the 15 kN load is 2 m below B) gives the base shear HA=MAB+MBA−15×26H_A=\dfrac{M_{AB}+M_{BA}-15\times2}{6}; for CD, HD=MCD+MDC6H_D=\dfrac{M_{CD}+M_{DC}}{6}. Horizontal equilibrium HA+HD+15=0H_A+H_D+15=0 then gives MAB+MBA6+MCD+MDC6+10=0\dfrac{M_{AB}+M_{BA}}{6}+\dfrac{M_{CD}+M_{DC}}{6}+10=0. When the member equations (which include the FEMs) are substituted, the constant on the right-hand side becomes 10+−6.67+13.336=11.1110+\dfrac{-6.67+13.33}{6}=11.11 kN. This equals the equivalent joint load at B, i.e. the fixed-end reaction of the loaded column at B, Pa2(L+2b)L3=15×42(6+4)63=11.11\dfrac{Pa^2(L+2b)}{L^3}=\dfrac{15\times4^2(6+4)}{6^3}=11.11 kN.
EI[2.46670.4000−0.41670.40002.1333−0.3333−0.4167−0.33330.2500]{θBθCΔ1}={73.333−66.66711.111}EI\begin{bmatrix}2.4667 & 0.4000 & -0.4167 \\ 0.4000 & 2.1333 & -0.3333 \\ -0.4167 & -0.3333 & 0.2500\end{bmatrix}\begin{Bmatrix}\theta_{B} \\ \theta_{C} \\ \Delta_{1}\end{Bmatrix}=\begin{Bmatrix}73.333 \\ -66.667 \\ 11.111\end{Bmatrix}

(Rows 1 and 2: joints B and C. Row 3: storey shear, right-hand side = 11.11 kN.)

Solution

EIθB=49.5343,EIθC=−26.1394,EIΔ1=92.1490EI\theta_{B}=49.5343,\quad EI\theta_{C}=-26.1394,\quad EI\Delta_{1}=92.1490

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

EndMM (kNm)EndMM (kNm)
AB-3.78BA57.50
BC-37.50CB65.57
CD-65.57DC-48.14

Checks:

  • Joint B: (57.50) + (-37.50) = 20.00 kNm (applied clockwise moment 20.00) ✓
  • Joint C: (65.57) + (-65.57) = 0.00 kNm (applied clockwise moment 0.00) ✓
MemberBM at first endBM at second endMax within member
AB-3.78-57.50-
BC-37.50-65.5748.96 at 4.65 m
CD-65.5748.14-

Reactions: A: H=3.95H=3.95, V=37.19V=37.19, M=3.78M=3.78; D: H=−18.95H=-18.95, V=42.81V=42.81, M=48.14M=48.14.

Answer: MAB=−3.78M_{AB}=-3.78, MBA=57.50M_{BA}=57.50, MBC=−37.50M_{BC}=-37.50, MCB=65.57M_{CB}=65.57, MCD=−65.57M_{CD}=-65.57, MDC=−48.14M_{DC}=-48.14 kNm.

✓ Answer checked by Claude Opus 5.5 (high effort)

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