Step 1: Set up the free body using the load P alone.
Take the fixed wall as \( x=0 \) and the free end as \( x=L \), with the downward load \( P \) at \( x=L/2 \).
For a cantilever with a point load at midspan, the shear stays at \( P \) from the wall up to the load, then drops to zero beyond it, since nothing pushes the beam past that point except the end moment.
Step 2: Get the bending moment due to P alone.
Cutting at any \( x \) between \( 0 \) and \( L/2 \) and looking at the segment beyond the cut, the moment needed to balance \( P \) grows linearly from \( 0 \) at \( x=L/2 \) to \( PL/2 \) at the wall \( (x=0) \).
Beyond the load point, from \( x=L/2 \) to \( x=L \), there is no more transverse force, so this part of the moment stays at \( 0 \).
Step 3: Add the effect of the applied end moment \( M=PL/2 \).
A pure moment applied at the tip adds no shear anywhere, since it has no force component, so the SFD stays exactly as in Step 1: \( P \) from \( 0 \) to \( L/2 \), then \( 0 \) to \( L \).
A pure end moment does add a constant bending moment across the whole span, and here it is sized and directed so it exactly cancels the \( PL/2 \) moment that the load alone creates at the wall.
Step 4: Add the two bending moment contributions.
At the wall, \( PL/2 \) (from \( P \)) minus \( PL/2 \) (from \( M \)) gives \( 0 \).
At the load point and beyond, the \( P \)-only moment is already \( 0 \), so only the constant \( PL/2 \) from \( M \) remains, all the way to the tip.
Final Answer:
The bending moment rises from \( 0 \) at the wall to \( PL/2 \) at midspan, then stays flat at \( PL/2 \) to the free end, while the shear stays \( P \) up to midspan and \( 0 \) after, matching option A.
\[ \boxed{\text{Option A}} \]