Let’s start by considering the reaction at point \( B \) due to the applied moment.
1. Reaction due to Moment:
The moment \( M \) applied at the cantilever results in a reaction force at point \( B \). Since the flexural rigidity \( EI \) is constant, the moment at the support \( B \) is given by:
\[
R_m = \frac{3M}{2L}
\]
2. Deflection at B:
The deflection at point \( B \) should be zero, thus:
\[
\frac{ML^2}{2EI} - R_m \times \frac{L^3}{3EI} = 0
\]
Substituting \( R_m = \frac{3M}{2L} \) into this equation:
\[
\frac{ML^2}{2EI} - \frac{3M}{2L} \times \frac{L^3}{3EI} = 0
\]
This simplifies to:
\[
R_m = \frac{3M}{2L}
\]
3. Reaction at Propped End Due to Sinking of Support:
The reaction at the propped end due to the sinking of the support is given by:
\[
R_{\Delta} = \frac{3EI}{L^3} \times \Delta
\]
4. Net Reaction at Propped End:
The net reaction at the propped end is the combination of the moment reaction and the sinking due to support movement. Therefore, the net reaction is:
\[
R_B = \frac{3M}{2L} - \frac{3EI}{L^3} \times \Delta
\]
Thus, the net upward reaction at the propped support \( B \) is given by:
\[
\boxed{ \frac{3M}{2L} - \frac{3EI}{L^3} \times \Delta }
\]