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Beam deflection and stresses at B (FEM)

Short answer

Using three beam elements and solving the assembled stiffness equations gives deflection at B: v_B = -230/EI m (downward). Bending moment at B is 38.75 kN m, so bending stress σ = 38.75×10^6 y / I N/mm^2 (tension bottom, compression top).

For the given beam determine the deflection at point B and the stresses at the same point.

[Figure: beam A-B-D-C of uniform EIEI; 10 kN/m uniformly distributed load over AB (4 m); B to D is 2 m with a 40 kN downward point load at D; D to C is 2 m; A fixed end, C supported at the right end]

Assumptions (figure data): A is fixed, C is a roller (simple support), EIEI is constant. Three beam elements: AB (4 m, 10 kN/m UDL), BD (2 m) and DC (2 m, no load); the 40 kN downward load acts at node D. Positive: vv upward, θ\theta counter-clockwise. Units: kN, m.

Element stiffness

Each element uses

[k]=EIL3[126L−126L6L4L2−6L2L2−12−6L12−6L6L2L2−6L4L2],{d}={vi,θi,vj,θj}T[k]=\frac{EI}{L^3}\begin{bmatrix}12&6L&-12&6L\\6L&4L^2&-6L&2L^2\\-12&-6L&12&-6L\\6L&2L^2&-6L&4L^2\end{bmatrix},\quad \{d\}=\{v_i,\theta_i,v_j,\theta_j\}^T

(Upward forces and displacements, and counter-clockwise moments and rotations, are positive.) with L=4L=4 m (AB), L=2L=2 m (BD, DC). Nodes: 1 = A, 2 = B, 3 = D, 4 = C.

Equivalent nodal loads

Element AB: wL/2=20wL/2=20 kN, wL2/12=13.333wL^2/12=13.333 kN m, so the equivalent loads are −20-20 kN and −13.333-13.333 kN m at A, and −20-20 kN and +13.333+13.333 kN m at B. The 40 kN load is a direct nodal load at D.

Assembled equation (free DOFs vB,θB,vD,θD,θCv_B,\theta_B,v_D,\theta_D,\theta_C)

With vA=θA=0v_A=\theta_A=0 and vC=0v_C=0:

EI [1.6881.125−1.5001.50001.1253.000−1.5001.0000−1.500−1.5003.00001.5001.5001.00004.0001.000001.5001.0002.000]{vBθBvDθDθC}={−20.00013.333−40.00000}EI\,\begin{bmatrix}1.688 & 1.125 & -1.500 & 1.500 & 0 \\ 1.125 & 3.000 & -1.500 & 1.000 & 0 \\ -1.500 & -1.500 & 3.000 & 0 & 1.500 \\ 1.500 & 1.000 & 0 & 4.000 & 1.000 \\ 0 & 0 & 1.500 & 1.000 & 2.000\end{bmatrix}\begin{Bmatrix}v_B\\\theta_B\\v_D\\\theta_D\\\theta_C\end{Bmatrix}=\begin{Bmatrix}-20.000 \\ 13.333 \\ -40.000 \\ 0 \\ 0\end{Bmatrix}

Solving:

vB=−230.00EI m,θB=−34.167EI radvD=−207.083EI m,θD=63.958EI rad,θC=123.333EI rad\begin{aligned} v_B&=-\frac{230.00}{EI}\ \text{m},&\theta_B&=-\frac{34.167}{EI}\ \text{rad}\\ v_D&=-\frac{207.083}{EI}\ \text{m},&\theta_D&=\frac{63.958}{EI}\ \text{rad},\quad \theta_C=\frac{123.333}{EI}\ \text{rad} \end{aligned}

Deflection at B = 230.0/EI m downward (with EIEI in kN m2^2; e.g. EI=2×104EI=2\times10^4 kN m2^2 gives 11.5 mm).

Element end forces {f}=[k]{d}−{Feq}\{f\}=[k]\{d\}-\{F_{eq}\}

ElementViV_i (kN)MiM_i (kN m)VjV_j (kN)MjM_j (kN m)
AB50.312582.500-10.312538.750
BD10.3125-38.750-10.312559.375
DC-29.6875-59.37529.68750.000

Reactions: RA=50.312R_A=50.312 kN (up), MA=82.50M_A=82.50 kN m (counter-clockwise), RC=29.687R_C=29.687 kN. Check: 50.3125+29.6875=8050.3125+29.6875=80 kN = 10×4+4010\times4+40.

Bending moment (sagging +) and shear force

  • A: −82.50-82.50 (hogging); at 2 m from A: −1.875-1.875; B: +38.75+38.75; D: +59.375+59.375; C: 00.
  • Shear: +50.31+50.31 at A, +10.31+10.31 at B (just before and after), −29.69-29.69 right of D.
 A(fixed)      B          D         C(roller)
 |-------------|----------|---------|
 BMD: -82.5   +38.75     +59.375     0   (kN m)
 SFD: +50.31 -> +10.31 (A to D) -> -29.69 (D to C)

Stresses at B

At B, MB=38.75M_B=38.75 kN m (sagging) and VB=10.31V_B=10.31 kN. The bending stress at a fibre at distance yy from the neutral axis is

σB=MB yI=38.75×106 yI N/mm2\sigma_B=\frac{M_B\,y}{I}=\frac{38.75\times10^6\ y}{I}\ \text{N/mm}^2

tension at the bottom and compression at the top. The section size is not given, so for a rectangular section b×hb\times h use σmax=6MB/(bh2)\sigma_{max}=6M_B/(bh^2); the average shear stress is τ=VB/A\tau=V_B/A (maximum 1.5VB/A1.5V_B/A for a rectangle).

Answer: vB=−230.00/EIv_B=-230.00/EI m (downward), θB=−34.167/EI\theta_B=-34.167/EI, MB=38.75M_B=38.75 kN m; σB=MBy/I\sigma_B=M_By/I.

✓ Answer checked by Claude Opus 5.5 (high effort)

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