Trigonometric Functions
One common application of sinusoidal functions, meaning functions that can be described by a sine or cosine equation, is harmonic motion. There are various types of harmonic motion, but we will focus on simple harmonic motion.
An object whose displacement or movement can be described using a sinusoidal function is said to follow simple harmonic motion. The displacement \(d\) of the object can be modeled as a function over time \(t\) using one of the formulas below.
\[\begin{align*} d &= a\sin(\omega t) \\ d &= a\cos(\omega t) \end{align*}\]The \(a\)-value is the amplitude, or maximum displacement of the object from rest. The \(\omega\)-value, "omega", is related to the period of the object's motion by the formula \(\omega = \frac{2\pi}{\text{period}}\), or by \(\text{period} = \frac{2\pi}{\omega}\). The frequency of the object's motion is the reciprocal of the period, so \(f = \frac{1}{\text{period}} = \frac{\omega}{2\pi}\), or \(\omega = 2\pi f\). We use sine if the object's initial position is at rest or at equilibrium, and we use cosine if its initial position is at its maximum displacement.
Don't let the new letters or context mix you up. We are still talking about sine and cosine graphs with amplitude \(a\), but we are not using \(\omega\) instead of \(k\). The frequency is really the only new thing. Let's wrap this lesson up by looking at a few examples.