Skip to main content

Stiffness method: frame, flexural deformations only

Short answer

Use stiffness method with no sway; unknowns are rotations at A and B. Solve equilibrium to get EI theta_A = -10.3448, EI theta_B = 20.6897. Final moments: M_AB=0, M_BA=12.41, M_BC=27.59, M_CB=13.79 kNm.

Analyze the frame shown in figure using the stiffness method (displacement method). Consider only flexural deformations and take EI as constant throughout. [Figure: frame; left column of 5 m, hinged at the base A (with 3 m dimension); 10 kN horizontal at B; beam BC of 3 m; C fixed with 40 kNm moment applied.]

Assumptions (figure partly described): the frame is A-B-C: column AB is 5 m high with a hinge at A; the beam BC is 3 m long, fixed at C. At joint B a 10 kN horizontal force (to the right) and a 40 kNm clockwise moment act. EI is constant and only flexural deformation is considered (axial and shear deformations neglected). Since C is fixed, B cannot translate horizontally; the vertical displacement of B is prevented by the column (axially rigid), so no sway occurs and the unknowns are the rotations θA\theta_A (hinge) and θB\theta_B (clockwise +).

Member stiffness equations (no member loads)

  • MAB=2EI5(2θA+θB)M_{AB}=\frac{2EI}{5}\left(2\theta_{A} + \theta_{B}\right)
  • MBA=2EI5(2θB+θA)M_{BA}=\frac{2EI}{5}\left(2\theta_{B} + \theta_{A}\right)
  • MBC=2EI3(2θB)M_{BC}=\frac{2EI}{3}\left(2\theta_{B}\right)
  • MCB=2EI3(θB)M_{CB}=\frac{2EI}{3}\left(\theta_{B}\right) The 10 kN force acts at the joint B and is carried directly to the supports by axial force in BC (it produces no bending moment).

Equilibrium

  • Hinge A: MAB=0M_{AB}=0
  • Joint B: MBA+MBC=40M_{BA}+M_{BC}=40 (applied clockwise moment)

Stiffness matrix equation

EI[0.80000.40000.40002.1333]{θAθB}={0.00040.000}EI\begin{bmatrix}0.8000 & 0.4000 \\ 0.4000 & 2.1333\end{bmatrix}\begin{Bmatrix}\theta_{A} \\ \theta_{B}\end{Bmatrix}=\begin{Bmatrix}0.000 \\ 40.000\end{Bmatrix}

K11=4EI5=0.8EIK_{11}=\dfrac{4EI}{5}=0.8EI, K12=2EI5=0.4EIK_{12}=\dfrac{2EI}{5}=0.4EI, K22=4EI5+4EI3=2.1333EIK_{22}=\dfrac{4EI}{5}+\dfrac{4EI}{3}=2.1333EI.

EIθA=−10.3448,EIθB=20.6897EI\theta_{A}=-10.3448,\quad EI\theta_{B}=20.6897

End moments (kNm, clockwise +)

EndMM (kNm)EndMM (kNm)
AB0.00BA12.41
BC27.59CB13.79

Checks: MAB=0.00M_{AB}=0.00 ✓; Joint B: 12.41+27.59=40.0012.41+27.59=40.00 kNm = applied 40 kNm ✓.

Reactions

A: H=2.48H=2.48, V=−13.79V=-13.79, M=0.00M=0.00; C: H=−12.48H=-12.48, V=13.79V=13.79, M=−13.79M=-13.79 (M anticlockwise +). Horizontally the supports give 2.48 kN at A (equal to the column shear caused by the end moments) and -12.48 kN at C; their sum balances the 10 kN load. The column shear is (MAB+MBA)/5=2.48(M_{AB}+M_{BA})/5=2.48 kN.

Bending moment diagram

MemberBM at first endBM at second endMax within member
AB0.00-12.41-
BC27.59-13.79-

Answer: MAB=0M_{AB}=0, MBA=12.41M_{BA}=12.41 kNm, MBC=27.59M_{BC}=27.59 kNm, MCB=13.79M_{CB}=13.79 kNm; θB=20.690/EI\theta_B=20.690/EI (clockwise).

✓ Answer checked by Claude Opus 5.5 (high effort)

All Theory of Structures II chapter 3 questions →