Step I: Analysis of motion: In this case the string rotates the pulley i.e., the string does not slide. The pulley will have angular acceleration. Hence, the tension on the string on both the sides of the pulley will not be equal. The motion of m1 and m2 will be translational. Positive direction of angular acceleration α is taken along the corresponding acceleration a1 which is taken positive in the direction of net force.
Step II: Equation of motion: Let these be T1 and T2. The equation of motion respectively, for masses m1 and m2 is
T1=m1a...(i)
m2g−T2=m2a....(ii)
Step III: Application of torque equation:
The torque equation for the pulley
T2R−T1R=Iα....(iii)
(N2 constitutes no torque about the axis of rotation)
There is no slipping of the string over the pulley
Step IV: Constraint relation
a=αR⇒α=aR...(iv)
From Eqs. (iii) and (iv) we get
∴T2R−T1R=IaRorT2−T1=IaR2...(v)
Step V: Solving equations:
Solving the above equations, we get a=m2gm1+m2+IR2
Here I=MR22
T1=m1m2g(m1+m2+IR2);T2=(m1+IR2)m2gm1+m2+IR2