The angular frequency of a simple harmonic oscillator is:
\[
\omega = \sqrt{\frac{k}{m}},
\]
where:
\begin{itemize}
\item \( k \) is the spring constant, which represents the stiffness of the spring.
\item \( m \) is the mass of the oscillator.
\end{itemize}
Derivation:
\begin{itemize}
\item The restoring force in SHM is \( F = -kx \), where \( x \) is displacement.
\item Using Newton’s second law \( F = ma \), where \( a = \ddot{x} \):
\[
m\ddot{x} + kx = 0.
\]
\item This is a second-order differential equation whose solution gives \( \omega = \sqrt{\frac{k}{m}} \).
\end{itemize}
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