Question 11.SP.7: For the uniform beam and loading shown, determine the reacti...

For the uniform beam and loading shown, determine the reactions at the supports.

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Castigliano’s Theorem. The beam is indeterminate to the first degree and we choose the reaction RA\mathbf{R}_{A} as redundant. Using Castigliano’s theorem, we determine the deflection at AA due to the combined action of RA\mathbf{R}_{A} and the distributed load. Since EIE I is constant, we write

yA=MEI(MRA)dx=1EIMMRAdxy_{A}=\int \frac{M}{E I}\left(\frac{\partial M}{\partial R_{A}}\right) d x=\frac{1}{E I} \int M \frac{\partial M}{\partial R_{A}} d x     (1)

The integration will be performed separately for portions ABA B and BCB C of the beam. Finally, RA\mathbf{R}_{A} is obtained by setting yAy_{A} equal to zero.

Free Body: Entire Beam. We express the reactions at BB and CC in terms of RAR_{A} and the distributed load

RB=94wL3RARC=2RA34wLR_{B}=\frac{9}{4} w L-3 R_{A} \quad R_{C}=2 R_{A}-\frac{3}{4} w L    (2)

Portion AB of Beam. Using the free-body diagram shown, we find

M1=RAxwx22M1RA=xM_{1}=R_{A} x-\frac{w x^{2}}{2} \quad \frac{\partial M_{1}}{\partial R_{A}}=x

Substituting into Eq. (1) and integrating from AA to BB, we have

1EIM1MRAdx=1EI0L(RAx2wx32)dx=1EI(RAL33wL48)\frac{1}{E I} \int M_{1} \frac{\partial M}{\partial R_{A}} d x=\frac{1}{E I} \int_{0}^{L}\left(R_{A} x^{2}-\frac{w x^{3}}{2}\right) d x=\frac{1}{E I}\left(\frac{R_{A} L^{3}}{3}-\frac{w L^{4}}{8}\right)    (3)

Portion BC of Beam. We have

M2=(2RA34wL)vwv22M2RA=2vM_{2}=\left(2 R_{A}-\frac{3}{4} w L\right) v-\frac{w v^{2}}{2} \quad \frac{\partial M_{2}}{\partial R_{A}}=2 v

Substituting into Eq. (1) and integrating from CC, where v=0v=0, to BB, where v=12Lv=\frac{1}{2} L, we have

1EIM2M2RAdv=1EI0L/2(4RAv232wLv2wv3)dv=1EI(RAL36wL416wL464)=1EI(RAL365wL464)(4) \begin{aligned} \frac{1}{E I} \int M_{2} \frac{\partial M_{2}}{\partial R_{A}} d v & =\frac{1}{E I} \int_{0}^{L / 2}\left(4 R_{A} v^{2}-\frac{3}{2} w L v^{2}-w v^{3}\right) d v \\ & =\frac{1}{E I}\left(\frac{R_{A} L^{3}}{6}-\frac{w L^{4}}{16}-\frac{w L^{4}}{64}\right)=\frac{1}{E I}\left(\frac{R_{A} L^{3}}{6}-\frac{5 w L^{4}}{64}\right) & (4) \end{aligned}

Reaction at A\boldsymbol{A}. Adding the expressions obtained in (3) and (4), we determine yAy_{A} and set it equal to zero

yA=1EI(RAL33wL48)+1EI(RAL365wL464)=0y_{A}=\frac{1}{E I}\left(\frac{R_{A} L^{3}}{3}-\frac{w L^{4}}{8}\right)+\frac{1}{E I}\left(\frac{R_{A} L^{3}}{6}-\frac{5 w L^{4}}{64}\right)=0

Solving for RA,RA=1332wLRA=1332wLR_{A}, \quad R_{A}=\frac{13}{32} w L \quad R_{A}=\frac{13}{32} w L \uparrow

Reactions at B\boldsymbol{B} and C\boldsymbol{C}. Substituting for RAR_{A} into Eqs. (2), we obtain

RB=3332wLRC=wL16R_{B}=\frac{33}{32} w L \uparrow \quad R_{C}=\frac{w L}{16} \uparrow

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