Published by Patrick Mutisya · 14 days ago
Simple harmonic motion (SHM) is a type of periodic motion where the restoring force is directly proportional to the displacement from an equilibrium position and acts in the opposite direction. It can be described mathematically by sinusoidal functions.
The displacement of an object undergoing SHM can be written as:
\$x(t) = A \cos(\omega t + \phi)\$
or equivalently, using a sine function:
\$x(t) = A \sin(\omega t + \phi)\$
Both forms describe the same motion; the choice of cosine or sine simply changes the initial phase.
The three quantities are interrelated:
\$T = \frac{1}{f}, \qquad \omega = 2\pi f, \qquad T = \frac{2\pi}{\omega}\$
These equations allow conversion between any two of the quantities.
| Quantity | Symbol | Unit | Definition / Relationship |
|---|---|---|---|
| Displacement | \$x\$ | metre (m) | Instantaneous distance from equilibrium |
| Amplitude | \$A\$ | metre (m) | Maximum displacement, \$|x|_{\max}\$ |
| Period | \$T\$ | second (s) | Time for one complete cycle |
| Frequency | \$f\$ | hertz (Hz) | \$f = 1/T\$ |
| Angular Frequency | \$\omega\$ | radian per second (rad s⁻¹) | \$\omega = 2\pi f = 2\pi/T\$ |
| Phase Difference | \$\phi\$ | radian (rad) | Angular offset between two SHM motions |
For a mass \$m\$ attached to a spring with force constant \$k\$, the angular frequency is given by:
\$\omega = \sqrt{\frac{k}{m}}\$
Consequently, the period and frequency become:
\$T = 2\pi\sqrt{\frac{m}{k}}, \qquad f = \frac{1}{2\pi}\sqrt{\frac{k}{m}}\$
If two pendulums of identical length are set into motion, and one starts \$30^\circ\$ (or \$\pi/6\$ rad) ahead of the other, the phase difference is \$\phi = \pi/6\$ rad. Their displacements can be written as:
\$x_1(t) = A \cos(\omega t)\$
\$x_2(t) = A \cos(\omega t + \phi)\$