Since the prompt says to determine the reactions and to use Castigliano's Theorem, it is likely referring to the method of least work. The beam is statically indeterminate. We will consider the reaction at B as the redundant reaction (RB). Castigliano's second theorem states:
δi=∂Pi∂U Where δi is the displacement in the direction of the force Pi and U is the strain energy. Since support B is a rigid support, the vertical displacement at B is zero. Therefore, δB=0. Thus, according to Castigliano's theorem:
∂RB∂U=0 The strain energy due to bending is given by:
U=∫2EIM2dx Therefore,
∂RB∂U=∫EIM∂RB∂Mdx=0 Or simply,
∫M∂RB∂Mdx=0 First, determine the support reactions at A and C. Let RA and RC be the vertical reactions at A and C, respectively. Sum of moments about C = 0: RA(14)−10(9)+RB(4)−2(4)(2)=0 14RA+4RB=90+16=106 RA=14106−4RB=753−2RB Sum of vertical forces = 0:
RA+RB+RC−10−2(4)=0 RA+RB+RC=18 RC=18−RB−RA=18−RB−(753−2RB)=7126−7RB−53+2RB=773−5RB Now we divide the beam into two sections, AB and BC.
For section AB (0 <= x <= 10), measuring from A:
M(x)=RAx−10(x−4)H(x−4)=(753−2RB)x−10(x−4)H(x−4) Where H(x-4) is the Heaviside step function (0 for x<4 and 1 for x>=4).
∂RB∂M=−72x For section BC (0 <= x <= 4), measuring from C:
M(x)=RCx−2x(2x)=(773−5RB)x−x2 ∂RB∂M=−75x The integration is performed as follows:
∫010M∂RB∂Mdx+∫04M∂RB∂Mdx=0 ∫010[(753−2RB)x−10(x−4)H(x−4)](−72x)dx+∫04[(773−5RB)x−x2](−75x)dx=0 −492∫010(53−2RB)x2dx+720∫410(x2−4x)dx−495∫04(73−5RB)x2dx+75∫04x3dx=0 −492(53−2RB)[3x3]010+720[3x3−2x2]410−495(73−5RB)[3x3]04+75[4x4]04=0 −492(53−2RB)31000+720[(31000−200)−(364−32)]−495(73−5RB)364+754256=0 −1472000(53−2RB)+720[3400+332]−147320(73−5RB)+75(64)=0 −1472000(53−2RB)+720[3432]−147320(73−5RB)+7320=0 −147106000+1474000RB+720(144)−14723360+1471600RB+7320=0 1475600RB=147106000+14723360−72880−7320 1475600RB=147129360−73200=147129360−67200=14762160 RB=14762160⋅5600147=560062160=11.1kN RA=753−2(11.1)=753−22.2=730.8=4.4kN RC=773−5(11.1)=773−55.5=717.5=2.5kN