168 CHAPTER 5 Energy Methods
Fig. P.5.24
giventhat
(a) thetemperaturedistributionis
θ=θ 0 cos2ψ for−π/ 4 <ψ<π/ 4
θ=0 for−π/ 4 >ψ>π/ 4
(b) bendingdeformationsonlyaretobetakenintoaccount:
α =coefficientoflinearexpansionofframematerial
EI=bendingrigidityofframe
h =depthofcrosssection
r =meanradiusofframe.