Castigliano's second theorem states that the partial derivative of the total strain energy with respect to an applied force is equal to the displacement at the point of application of that force in the direction of that force. Since the supports A, B, and C are fixed, the vertical displacement at each support is zero. Thus, we can apply Castigliano's theorem to find the reactions at the supports.
Let RA, RB, and RC be the reactions at supports A, B, and C, respectively. Since we have three unknowns and only two equations of equilibrium, we need to use Castigliano's theorem to obtain a third equation. ∂RA∂U=0 ∂RB∂U=0 ∂RC∂U=0 U=∫0L2EIM(x)2dx First, consider the free body diagram of the beam. Summing vertical forces:
RA+RB+RC=10+2∗4=18 kN Summing moments about A:
RB∗6+RC∗10=10∗4+2∗4∗(6+4/2)=40+8∗8=40+64=104 kNm We now use Castigliano's theorem. Consider the moment at a distance x from A. M(x)=RAx−10⟨x−4⟩1 For 6<x<10: M(x)=RAx−10⟨x−4⟩1+RB(x−6) Where ⟨x−a⟩n=(x−a)n if x>a and 0 if x<a. U=∫0102EIM2dx We differentiate with respect to RA: ∂RA∂U=∫0102EI2M∂RA∂Mdx=∫010EIM∂RA∂Mdx=0 ∂RA∂M=x ∫010Mxdx=0 ∫06(RAx−10⟨x−4⟩)xdx+∫610(RAx−10⟨x−4⟩+RB(x−6))xdx=0 ∫06(RAx2−10x(x−4))dx+∫610(RAx2−10x(x−4)+RBx(x−6))dx=0 ∫04RAx2dx+∫46(RAx2−10x(x−4))dx+∫610(RAx2−10x(x−4)+RBx(x−6))dx=0 ∫04RAx2dx+∫46(RAx2−10x2+40x)dx+∫610(RAx2−10x2+40x+RBx2−6RBx)dx=0 [RA3x3]04+[RA3x3−310x3+20x2]46+[RA3x3−310x3+20x2+RB3x3−3RBx2]610=0 RA364+RA(3216−364)−310(216−64)+20(36−16)+RA(31000−3216)−310(1000−216)+20(100−36)+RB(31000−3216)−3RB(100−36)=0 RA364+RA3152−310∗152+400+RA3784−310∗784+20∗64+RB3784−3RB(64)=0 RA(364+152+784)+RB(3784−192)=310∗152−400+310∗784−1280 RA(31000)+RB(3784−576)=31520+7840−1680 31000RA+3208RB=39360−5040 1000RA+208RB=4320 125RA+26RB=540 We have RA+RB+RC=18 and 6RB+10RC=104. Then RC=10104−6RB. RA+RB+10104−6RB=18 10RA+10RB+104−6RB=180 10RA+4RB=76 5RA+2RB=38 We also have 125RA+26RB=540. Multiply the first equation by