Two identical atoms of mass \( m \) are bound to each other by the Lennard-Jones potential,
\[
V = \varepsilon \left[ \left( \frac{r_0}{r} \right)^{12} - 2 \left( \frac{r_0}{r} \right)^6 \right]
\]
The frequency of small oscillations about the equilibrium is:
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The Lennard-Jones potential describes interatomic interactions, including bonding forces.
Expanding \( V(r) \) about equilibrium \( r = r_0 \) and using harmonic approximation:
\[
\omega = \sqrt{\frac{V''(r_0)}{m}}
\]
After differentiating and solving:
\[
\omega = \sqrt{\frac{12\varepsilon}{m r_0^2}}
\]