Recall that F = - kx . Thus the force on the mass will be greatest when the displacement of the block is maximum, or when x = ±x _m .

We have derived that T = 2Π . To find the period of oscillation we simply plug into this equation:

No matter what initial conditions are placed on the system ,the period of oscillation will be same. Notice again that period, frequency and angular frequency are properties of the system, not of the conditions placed on the system.

For this problem we use the sin and cosine equations we derived for simple harmonic motion. Recall that x = x _mcos(σt) . We are given x and x _m in the question, and must calculate σ before we can find t . We know, however, that no matter the initial displacement, σ = = = = 3 . Thus we can plug in our values:

This problem was a simple example of how to use our equations for simple harmonic motion.

To find the period of oscillation we need only know m and k . We are given m and must find k for the spring. If a 4 kg mass oscillates with a period of 2 seconds, we can calculate k from the following equation:

Implying that

Now that we have k , calculating the period for a different mass is easy:

A general statement can be made from this problem: a larger mass attached to a given spring will oscillate with a longer period.

When the mass is at its equilibrium point, no potential energy is stored in the spring. Thus all of the energy of the system is kinetic, and can be calculated easily:

Since this is the total energy of the system, we can use this answer to calculate the maximum displacement of the mass. When the block is maximally displaced, it is at rest and all of the energy of the system is stored as potential energy in the spring, given by U = kx _m ² . Since energy is conserved in the system, we can relate the answer we got for the energy at one position with the energy at another:

We used energy considerations in this problem in much the same way we did when we first encountered conservation of energy- whether the motion is linear, circular or oscillatory, our conservation laws remain powerful tools.