Our general equation for position in SHM is:

x(t) = A cos(ωt + δ)

Let's take this equation apart to analyze each piece separately.

Change the amplitude of the oscillation

For simple harmonic motion the oscillation frequency is independent of the amplitude. For instance, two equal masses connected to identical springs and released from rest at different points have the same angular frequency.

Change the frequency of oscillation

For a spring-mass system, frequency is changed by changing k/m, because ω = (k/m)^½. If we kept the k's the same but doubled one mass, for instance, frequency is reduced by a factor of the square root of two.

Change the phase

If all that is different is the phase, the graphs of x(t) are identical except that one is shifted relative to the other by the phase angle.