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Beam deflection at B, rotations (2 elements)

Short answer

Discretise into two 5 m beam elements with fixed and roller supports; solve the reduced stiffness equations. Deflection at B is 1041.67/EI downward, rotation at B is 104.17/EI clockwise, and rotation at C is 416.67/EI anticlockwise.

For the given beam find the deflection at point B and rotations at points B and C. Take EIEI as constant throughout the beam. Discretise the beam into two elements.

[Figure: beam A-B-C with 20 kN/m UDL over the whole length; AB = 5 m, BC = 5 m; A fixed at the left end, C roller supported]

The beam is divided into element 1 (A-B) and element 2 (B-C), each 5 m long, with nodes A, B, C. Dofs per node: (deflection vv, rotation θ\theta). A is fixed (vA=θA=0v_A=\theta_A=0) and C is a roller (vC=0v_C=0), so the unknowns are vB, θB, θCv_B,\ \theta_B,\ \theta_C.

  20 kN/m
 +++++++++++++++++++++++
 |===========o==========o   A fixed, C roller
 A           B          C
 |<--- 5 --->|<--- 5 -->|

Element stiffness (L=5L=5 m)

[k]=EI125[1230−123030100−3050−12−3012−303050−30100][k]=\frac{EI}{125}\begin{bmatrix}12&30&-12&30\\30&100&-30&50\\-12&-30&12&-30\\30&50&-30&100\end{bmatrix}

Equivalent nodal loads (per element)

wL/2=20×5/2=50wL/2=20\times5/2=50 kN, wL2/12=20×25/12=41.667wL^2/12=20\times25/12=41.667 kNm.

  • Element 1: (−50, −41.667, −50, +41.667)(-50,\ -41.667,\ -50,\ +41.667)
  • Element 2: same.

Loads on the free dofs (vB,θB,θC)(v_B,\theta_B,\theta_C): FvB=−50−50=−100F_{v_B}=-50-50=-100 kN, FθB=+41.667−41.667=0F_{\theta_B}=+41.667-41.667=0, FθC=+41.667F_{\theta_C}=+41.667 kNm.

Assembled equations for the free dofs

EI[0.19200.2401.60.40.240.40.8][vBθBθC]=[−100041.667]EI\begin{bmatrix}0.192&0&0.24\\0&1.6&0.4\\0.24&0.4&0.8\end{bmatrix}\begin{bmatrix}v_B\\ \theta_B\\ \theta_C\end{bmatrix}=\begin{bmatrix}-100\\0\\41.667\end{bmatrix}

Solution

vB=−1041.67EI,θB=−104.17EI rad (clockwise),θC=+416.67EI rad (anticlockwise)v_B=-\frac{1041.67}{EI},\qquad \theta_B=-\frac{104.17}{EI}\ \text{rad (clockwise)},\qquad \theta_C=+\frac{416.67}{EI}\ \text{rad (anticlockwise)}

Check with reactions and moments

{R}=[K]{d}−{F}\{R\}=[K]\{d\}-\{F\} gives RA=125R_A=125 kN, MA=250M_A=250 kNm and RC=75R_C=75 kN. ΣFy\Sigma F_y: 125+75=200=20×10125+75=200=20\times10 and ΣMA\Sigma M_A: 75×10−200×5+250=075\times10-200\times5+250=0 (with MAM_A anticlockwise). These agree with the propped-cantilever results RC=3wL/8=75R_C=3wL/8=75 kN, RA=5wL/8=125R_A=5wL/8=125 kN, MA=wL2/8=250M_A=wL^2/8=250 kNm.

Answer: deflection at B =1041.67/EI=1041.67/EI downward; rotations θB=104.17/EI\theta_B=104.17/EI (clockwise) and θC=416.67/EI\theta_C=416.67/EI (anticlockwise).

Bending moment: M(x)=−250+125x−10x2M(x)=-250+125x-10x^2 (sagging +). MA=−250M_A=-250, MB=+125M_B=+125 kNm, zero at x=2.5x=2.5 m, maximum +140.6+140.6 kNm at x=6.25x=6.25 m, MC=0M_C=0.

✓ Answer checked by Claude Opus 5.5 (high effort)

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