Let
w1 be the acceleration of mass
m1 and
w2 is the acceleration of mass
m2.Using Newton's second law in projection form along x-axis for the body 1 and along negative x-axis for the body 2 respectively, we get
m1g−T1=m1w1 (1)
T2−m2g=m2w2 (2)
For the pulley lowering in downward direction from Newton's law along x-axis,
T1−2T2=0 (as pulley is mass less)
or,
T1=2T2 (3)
As the length of the thread is constant so,
w2=2w1 (4)
The simultaneous solution of above equation yields,
w2=2(m1−2m2)g4m2+m1=2(η−2)η+4 (as
m1m2=η)
Obviously during the time interval in which the body 1 comes to the horizontal floor covering the distance
h, the body 2 moves upward the distance
2h. At the moment when the body 2 is at the height
2h from the floor its velocity is given by the expression:
v22=2w2(2h)=2[2(η−2)η+4]2h=8h(η−2)gη+4After the body
m1 touches the floor the thread becomes slack or the tension in the thread zero, thus as a result body 2 is only under gravity for it's subsequent motion.
Owing to the velocity
v2 at that moment or at the height
2h from the floor, the body 2 further goes up under gravity by the distance,
h′=v222g=4h(η−2)η+4Thus the sought maximum height attained by the body 2:
H=2h+h′=2h+4h(η−2)η+4=6ηhη+4