Here, m1 = 2 kg, m2 = 3 kg and m3 = 5 kg
(a) When the system is moving upward with an acceleration 'a' where a = 2 ms-2.
As per the fig., consider the free body diagram of the system of three blocks. Then,
T1 - (m1 + m2 + m2) g = (m1 + m2 + m3) a
or, T1 = (m1 + m2 + m3) (a + g) ...(i)
or, T1 = (2 + 3 + 5) x (2 x 9.8) = 118 N
Consider the free body diagram of blocks of masses m2 and m3. Then
T2 - (m2 + m3)g = (m2 + m3) x a ....(ii)
or, T2 = (m2 + m3)(a + g)
⇒ T2 = (3 + 5) x (2 x 9.8) = 94.4 N
Consider the free body diagram of block of mass m3. Then,
T3 - m3g = m3a ....(iii)
or, T3 = m3(g + a) = 5 x (2 + 9.8) = 59 N
(b) When the system is held stationary:
Obviously, a = 0, setting a = 0, in the equations (i), (ii) and (iii), we have
T1 = (m1 + m2 + m3) g = (2 + 3 + 5) x 9.8
= 98 N
T2 = (m2 + m3) g = (3 + 5) x 9.8 = 78.4 N
and T3 = m3g = 5 x 9.8 = 49 N