Castigliano's second theorem states that the partial derivative of the total strain energy U with respect to a force P is equal to the displacement at the point of application of the force in the direction of the force. Mathematically, ∂P∂U=Δ. For supports, we seek the reaction force, and the displacement is zero. Thus ∂RB∂U=0. We'll assume constant EI. The strain energy U is given by: U=∫2EIM2dx Therefore, ∂RB∂U=∫2EI2M∂RB∂Mdx=EI1∫M∂RB∂Mdx=0 Since EI is constant and not zero, we need to find the bending moment M as a function of x, then take its partial derivative with respect to RB, and finally integrate M∂RB∂M over the length of the beam. We will consider two sections: Section 1: AB and Section 2: BC. First, we need to determine the support reactions. Let's denote the vertical reactions at A, B, and C as RA, RB, and RC, respectively. Taking the sum of vertical forces to be zero gives: RA+RB+RC=10+2=12 Taking moments about point A:
6RB+11RC=10∗4+2∗6=40+12=52 Now, we introduce a dummy variable RB at support B. For section AB (0 <= x <= 6), taking moments about the cut at a distance x from A:
M1(x)=RAx−10⟨x−4⟩1, where ⟨x−a⟩n is the Macaulay bracket, equal to (x−a)n when x>a and 0 when x<a. For section BC (0 <= x' <= 5), taking moments about the cut at a distance x' from C:
M2(x′)=RCx′−2x′, where x' is the distance from C. Note that x′=11−x. RA+RB+RC=12 6RB+11RC=52 RA=12−RB−RC RC=(52−6RB)/11 RA=12−RB−(52−6RB)/11=(132−11RB−52+6RB)/11=(80−5RB)/11 M1(x)=11(80−5RB)x−10⟨x−4⟩1 M2(x′)=11(52−6RB)x′−2x′ ∂RB∂M1=11−5x ∂RB∂M2=11−6x′ ∫06(11(80−5RB)x−10⟨x−4⟩1)(11−5x)dx+∫05(11(52−6RB)x′−2x′)(11−6x′)dx′=0 ∫06(121−400x2+25RBx2+1150x⟨x−4⟩1)dx+∫05(121−312x′2+36RBx′2+132x′2)dx′=0 ∫06(121−400x2+25RBx2+1150x(x−4))dx from 4 to 6 +∫05(121−180x′2+36RBx′2)dx′=0 (121−400x3/3+25RBx3/3)∣06+(1150(x3/3−2x2))∣46+(121−180x′3/3+36RBx′3/3)∣05=0 (121−400∗216/3+25RB∗216/3)+(1150(216/3−2∗36)−50(64/3−2∗16))+(121−180∗125/3+36RB∗125/3)=0 (121−28800+1800RB)+(1150(72−72)−50(64/3−32))+(121−7500+1500RB)=0 (121−28800+1800RB)+(110−50(64/3−96/3))+(121−7500+1500RB)=0 (121−28800+1800RB)+(11−50(−32/3))+(121−7500+1500RB)=0 (121−28800+1800RB)+(111600/3)+(121−7500+1500RB)=0 (121−28800+1800RB)+(331600)+(121−7500+1500RB)=0 Multiplying by 121:
−28800+1800RB+1600∗121/33−7500+1500RB=0 −36300+3300RB+1600∗11/3=0 3300RB=36300−17600/3∗3/3=(108900−17600)/3=91300/3 RB=(91300/3)/3300=91300/(3∗3300)=91300/9900=913/99≈9.22