Let's first find the equilibrium position of the spring. When the mass is first attached the spring will oscillate like a simple harmonic oscillator, in the real world the oscillator will eventually settle and this position will be the new equilibrium position of the oscillator. Let's make the velocity 0 and resolve Newton's Second Law vertically (N2L from here on in): For a spring F=kx, N2L vertically kx=mg. Yielding x=mg/k where g is the local acceleration due to gravity.
For the Equation of Motion, resolve N2L while the oscillator is in motion. To make life easier lets substitute x = x0+y where x0 is the new equilibrium position as this way we don't need to worry about any constants and can have y oscillate around y=0. Now: ma=-kx where a = d^2x/dt^2. Solving this differential equation we get y = Acos(wt) + Bsin(wt) where we find that w^2 = k/m. Knowing that w=2pif we can work out the frequency of these oscillations.
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