When spring is equilibrium then
\(F = kx\)
\(mg = kx\)
\(x = \frac{mg} k\)
when spring compressed by 2x0
\(F = k(2x_0)-mg\)
\(ma = k2x_0 - mg\)
\(a = \frac{2kx_0}{m} - g\)
\(\because \frac{kx_0}m = g\)
\(a = \frac{kx_0}m\) .....(1)
\(a = -w^2x\) ......(2)
Comparing equation (1) and (2)
\(w^2 = \frac km\)
\(w = \sqrt{\frac km}\)
\(\frac{2\pi}{T} = \sqrt{\frac km}\)
\(2\pi \sqrt {\frac mk} = T\) .....(3)
\(kx_0 = mg\)
\(\frac{x_0}g = \frac mk\) -this put in equation (3)
\(T = 2\pi \sqrt {\frac mk}\)
\(T = 2\pi \sqrt{\frac{x_0}g}\)