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Consistent deformation: chair-frame with couple

Short answer

Release E; redundants H_E=9.22 kN, V_E=5.32 kN, M_E=-8.24 kNm. Bending moments: A=13.03, C left=-19.95, C right=30.05 kNm. Shear and axial constant per member; AB and CD 5.32 kN compression, BC and DE 9.22 kN tension.

Use the consistent deformation method to draw bending moment diagram of the chair-frame loaded with a couple as shown. Take E=2×104E = 2\times10^{4} MPa, ℓ=3\ell = 3 m, M=50M = 50 kNm and I=4.5×108 mm4I = 4.5\times10^{8}\ \text{mm}^4. Also draw shear force and normal thrust diagrams corresponding to the bending moment diagram. [Figure: chair-shaped frame; fixed top support, vertical member (2I) of height ℓ\ell, horizontal member (I) of length ℓ/3\ell/3 with the couple M applied at its end, then vertical member (2I) of height ℓ\ell and horizontal span 2ℓ/32\ell/3 down to a fixed base.]

Assumptions (the figure is only described): the chair frame is A(0,6) - B(0,3) - C(1,3) - D(1,0) - E(3,0) with ℓ=3\ell=3 m: AB vertical 2I2I (3 m), BC horizontal II (ℓ/3=1\ell/3=1 m), CD vertical 2I2I (3 m) and DE horizontal II (2ℓ/3=22\ell/3=2 m). A (top) and E (base) are fixed. The couple M=50M=50 kNm acts clockwise at joint C. Axial deformation is neglected. E=2×104E=2\times10^4 MPa =2×107=2\times10^7 kN/m², I=4.5×108I=4.5\times10^8 mm⁴ =4.5×10−4=4.5\times10^{-4} m⁴, so EI=9000EI=9000 kNm² and 2EI=180002EI=18000 kNm². Only the relative stiffnesses matter for the redundants, so EI is a common factor.

Degree of indeterminacy

Ds=6−3=3D_s=6-3=3. Release E and take X1=HEX_1=H_E (right +), X2=VEX_2=V_E (up +), X3=MEX_3=M_E (anticlockwise +) as redundants. The primary structure is the cantilever A-B-C-D-E fixed at A.

Moments in the primary structure (kNm)

Sectionm1m_1 (H=1)m2m_2 (V=1)m3m_3 (M=1)MLM_L
A (AB)6.003.001.00-50.00
B (AB)3.003.001.00-50.00
B (BC)3.003.001.00-50.00
C (BC)3.002.001.00-50.00
C (CD)3.002.001.000.00
D (CD)0.002.001.000.00
D (DE)0.002.001.000.00
E (DE)0.000.001.000.00

The couple at C acts on the part between the support A and C, so in the primary structure it produces a constant moment of 50 kNm on AB and BC (the sign is negative here) and no moment on CD and DE. Sign: positive = tension on the right-hand side when travelling A, B, C, D, E.

Flexibility matrix (∫mimj ds/EI\int m_im_j\,ds/EI, shown in units of 1/EI where EIEI is the stiffness of II)

[F]=1EI[45.0032.2512.0032.2528.5012.0012.0012.006.00],{ΔL}=1EI{−487.50−350.00−125.00}[F]=\frac{1}{EI}\begin{bmatrix}45.00&32.25&12.00\\32.25&28.50&12.00\\12.00&12.00&6.00\end{bmatrix},\qquad \{\Delta_L\}=\frac{1}{EI}\begin{Bmatrix}-487.50\\-350.00\\-125.00\end{Bmatrix}

Consistent deformation (E is fixed)

[F]{X}=−{ΔL}⇒X1=9.220 kN,X2=5.319 kN,X3=−8.245 kNm[F]\{X\}=-\{\Delta_L\}\Rightarrow X_1=9.220\ \text{kN},\quad X_2=5.319\ \text{kN},\quad X_3=-8.245\ \text{kNm}

Reactions at A

HA=−9.220H_A=-9.220 kN, VA=−5.319V_A=-5.319 kN, MA=−13.032M_A=-13.032 kNm (anticlockwise +). Check: ∑H=0\sum H=0, ∑V=0\sum V=0 ✓; moment equilibrium holds with the applied 50 kNm couple.

Bending moment diagram (kNm, sign as above)

SectionBM
A13.03
B-14.63
C (left, on BC)-19.95
C (right, on CD)30.05
D2.39
E-8.24

The jump at C (50.00 kNm) equals the applied couple. Every member has a straight-line BM because there are no loads along the members.

Shear force and normal thrust diagrams

MemberAxial N (+ tension)Shear at startShear at end
AB-5.32-9.22-9.22
BC9.22-5.32-5.32
CD-5.32-9.22-9.22
DE9.22-5.32-5.32

Shear and axial force are constant along each member. Axial: negative = compression. AB and CD carry 5.32 kN compression, while BC and DE carry 9.22 kN tension. The shear in each member equals the slope of its BM diagram, i.e. the change in BM along the member divided by the member length.

Answer: HE=9.22H_E=9.22 kN, VE=5.32V_E=5.32 kN, ME=−8.24M_E=-8.24 kNm; MA=13.03M_A=13.03 kNm, MC=(−19.95,30.05)M_C=(-19.95, 30.05) kNm.

✓ Answer checked by Claude Opus 5.5 (high effort)

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