Determine the reactions at the supports for the prismatic beam and load shown (Fig. 11.41a).
The beam is statically indeterminate to the first degree. The reaction at A is redundant and the beam is released from that support. The reaction R _A is considered to be an unknown load (Fig. 11.41b) and will be determined under the condition that the deflection y_A at A must be zero. By Castigliano’s theorem, y_A=\partial U / \partial R_A , where U is the strain energy of the beam under the distributed load and the redundant reaction. Recalling Eq. (11.57),
x_j=\frac{\partial U}{\partial P_j}=\int_0^L \frac{M}{E I} \frac{\partial M}{\partial P_j} d x (11.57)
y_A=\frac{\partial U}{\partial R_A}=\int_0^L \frac{M}{E I} \frac{\partial M}{\partial R_A} d x (1)
The bending moment M for the load of Fig. 11.41b at a distance x from A is
M=R_A x-\frac{1}{2} w x^2 (2)
and its derivative with respect to R_A is
\frac{\partial M}{\partial R_A}=x (3)
Substituting for M and \partial M / \partial R_A from Eqs. (2) and (3) into Eq. (1), write
y_A=\frac{1}{E I} \int_0^L\left(R_A x^2-\frac{1}{2} w x^3\right) d x=\frac{1}{E I}\left(\frac{R_A L^3}{3}-\frac{w L^4}{8}\right)
Set y_A=0 \text { and solve for } R_A :
R_A=\frac{3}{8} w L \quad R _A=\frac{3}{8} w L \uparrow
From the conditions of equilibrium for the beam, the reaction at B consists of the force and couple:
R _B=\frac{5}{8} w L \uparrow \quad M _B=\frac{1}{8} w L^2 ⤸