Find the constraint relation between the acceleration of the ring and the block. Measure the distances of ring and the block from the fixed pulley B.

(a) Suppose in a small time interval ∆t the ring is displaced from A to A′ and the block from C to C′. Drop a perpendicular A′P from A′ to AB. For small displacement A′B = PB. Since the length of the string is constant,
we have AB + BC = A'B + BC'
or, AP + PB + BC = A'B + BC
or, AP = B'C - BC = CC' (as A'B = PB)
or, AA'cosθ = CC'
or, \(\frac{AA'\cos\theta}{\Delta t} = \frac{CC'}{\Delta t}\)
or, (velocity of the ring) cosθ = (velocity of the block).
(b) If the initial acceleration of the ring is a, that of the block will be a cosθ . Let T be the tension in the string at this instant. Consider the block as the system. The forces acting on the block are
(i) Mg downward due to earth, and
(ii) T upward due to string.
equation of motion of the block is
Mg-T = Macosθ ... (i)
Now, consider the ring as the system. The forces acting on the ring are
(i) Mg downward due to gravity,
(ii) N upward due to the rod,
(iii) T along the string due to string.
Taking components along the rod, the equation of motion of the ring is
Tcosθ = ma ......(ii)
From (i) and (ii),
