




To analyze the problem, we need to understand the motion of the ball in the semi-spherical vessel and how forces act on it.
Concepts Involved:
Forces at Point \( Q \):
Energy Conservation:
Using energy conservation between point \( P \) and \( Q \):
m \cdot g \cdot h = \frac{1}{2} \cdot m \cdot v^2
where \( h = r(1 - \cos(\alpha)) \) is the vertical height.
v^2 = 2 \cdot g \cdot r \cdot (1 - \cos(\alpha))
Ratio of Forces:
The ratio \( A \) of centripetal force \( F_c \) to normal reaction \( N \) is:
A = \frac{F_c}{N} = \frac{m \cdot v^2 / r}{m \cdot g \cdot \cos(\alpha) - m \cdot v^2 / r}
Substituting \( v^2 \):
A = \frac{2g(1 - \cos(\alpha))}{g \cdot \cos(\alpha) - 2g(1 - \cos(\alpha))}
The graph of \( A \) versus \( \alpha \) will involve looking at this relationship as \( \alpha \) changes from 0 to \(\frac{\pi}{2}\).

The options given suggest that the correct graph is the one where \( A \) varies with \( \alpha \) reaching a maximum and then decreasing. The logical interpretation from the formula indicates such a trend.