The angular frequency \( \omega \) of a simple harmonic oscillator is determined by the equation:
\[
\omega = \sqrt{\frac{k}{m}},
\]
where \( k \) signifies the spring constant, indicating the spring's rigidity, and \( m \) represents the oscillator's mass.
Derivation:
The process begins with the restoring force in simple harmonic motion, given by \( F = -kx \), where \( x \) is the displacement.
Applying Newton's second law, \( F = ma \), with \( a = \ddot{x} \), yields:
\[
m\ddot{x} + kx = 0.
\]
This second-order differential equation's solution directly provides the angular frequency as \( \omega = \sqrt{\frac{k}{m}} \).