(a) If l is the extension produced in the spring then elastic force developed in the spring is balanced by applied force F.
We have F = kl,
or, l = F/k ....(i)
Again F = ma = md2y/dt2
Hence, md2y/dt2 = -ky [displacement of mass, y = l]
(Negative sign has been introduced as the direction of elastic force is opposite to the direction of displacement y).
or, d2y/at2 = -(K/m)y = -w2y ....(iii)
where ω2 = k/m
or, ω = √{k/m} ....(iv)
Equation (iii) shows that motion of mass 'm' is simple harmonic whose time period is given by:
T = 2π/ω = 2π/√{k/m} = 2π√{m/k} ...(v)
Further from equation (i) extension produced in the spring,
l = F/k
(b) In this case displacement of each mass,
y = 1/2
or displacement, y = {F/k}/{2} = F/2k
or, F = 2ky ...(vi)
Also, as F = m.d2y/dt2 ....(vii)
Hence, from (vi) and (vii),
m.d2y/dt2 = -2ky
(Again, negative sign is introduced as the direction of elastic force is opposite to direction of displacement y).
or, d2y/dt2 = -(2k/m)y
= ω2y ....(viii)
where ω2 = 2k/m
or, ω = √{2k/m}
Thus, we again find from equation (viii) that here also masses execute simple harmonic motion, whose time period is given by
T = 2π/ω = 2π/√{2k/m}
= 2π m/2k