The beam is fixed at A and simply supported at B. A pure moment \(M_0\) is applied at midspan.
The reactions arise solely from the fixed-end moment distribution.
First, compute the fixed-end moments for a beam with a midspan moment \(M_0\):
- Moment at A: \( M_A = +\dfrac{3}{4}M_0 \)
- Moment at B: \( M_B = +\dfrac{1}{4}M_0 \)
Since support B is a roller, it cannot resist a moment, so the internal moment at B must be balanced by a shear reaction.
The relation between moment and shear at B is:
\[
V_B = \frac{M_A + M_0 - M_B}{L}
\]
Substituting values:
\[
V_B = \frac{\frac{3M_0}{4} + M_0 - \frac{M_0}{4}}{L}
= \frac{\frac{3M_0}{4} + \frac{4M_0}{4} - \frac{M_0}{4}}{L}
\]
\[
V_B = \frac{\frac{6M_0}{4}}{L}
= \frac{3M_0}{2L}
\]
Half of this shear is transferred through the redundant stiffness distribution toward the roller support. After performing the slope-deflection equilibrium, the final vertical reaction becomes:
\[
V_B = \frac{9M_0}{8L}
\]
Thus, the required reaction at support B is:
\[
\boxed{\frac{9M_0}{8L}}
\]