SHM happens when the restoring acceleration is always directed back toward a fixed point and its magnitude is directly proportional to the displacement from that point.
Mathematically: \$a = -\omega^2 x\$ 🎢
| Variable | Meaning |
|---|---|
| \$x\$ | Displacement from equilibrium |
| \$a\$ | Acceleration |
| \$\omega\$ | Angular frequency (rad/s) |
The negative sign shows the acceleration is opposite to the displacement direction.
In a mass‑spring system: \$F = -kx\$ → \$a = -\frac{k}{m}x\$ → \$\omega = \sqrt{\frac{k}{m}}\$
Think of a playground swing. When you push it forward (displacement), gravity pulls it back (restoring force). The further you push, the stronger the pull back, just like SHM.
When you let go, the swing oscillates back and forth, slowing down gradually due to air resistance. The ideal SHM assumes no resistance. 🚀
Remember: The defining condition for SHM is \$a \propto -x\$.
When solving problems, first check if the restoring force is linear in displacement. If yes, you can write the differential equation and find the angular frequency.
Also, be careful with units: \$\omega\$ is in rad/s, not Hz. Convert using \$f = \frac{\omega}{2\pi}\$ if needed. 📐