Two blocks of masses m1=3m and m2=m are attached to the ends of a string which passes over a frictionless fixed pulley (which is a uniform disc of mass M=2m and radius R) as shown in Fig. The masses are then released. The acceleration of the system is
2g5
Refer to Fig. Since the pulley has a finite mass, two tensions T1 and T2 will not be equal. If a is the acceleration of the system, the equations of motion of masses are
m1g−T1=m1a⇒3mg−T1=3ma (1) and
(T2−m2g=m2a⇒T2−mg=ma (2)
The resultant tension (T1−T2) exerts a torque on the pulley which is given by
t=(T1−T2)R (3)
Also, t=Iα where I=12MR2 and α is the angular acceleration which is given by α=aR
∴t=12MR2×aR=12MRa=mRa (4)
(∵M=2m)
From Eqs. (3) and (4) we get
T2−T2=ma (5)
Using Eqs. (1) and (2) and (5) and solving for a we get a=2g5.