Oscillations of Spring — Core Principles
Core Principles
Oscillations of a spring-mass system are a classic example of Simple Harmonic Motion (SHM). A mass 'm' attached to an ideal spring with spring constant 'k' undergoes periodic back-and-forth motion when displaced from its equilibrium position.
This motion is governed by Hooke's Law, , where the restoring force is proportional to the displacement 'x' and acts opposite to it. This leads to an acceleration , which is the defining equation for SHM.
The angular frequency of oscillation is , and the period is . The frequency is . The period is independent of the amplitude for ideal SHM. Energy in the system continuously transforms between kinetic energy () and elastic potential energy (), with the total mechanical energy remaining constant.
Maximum velocity occurs at equilibrium, and maximum acceleration occurs at the extreme positions. Springs can be combined in series () or parallel (), affecting the system's period.
Important Differences
vs Simple Pendulum Oscillations
| Aspect | This Topic | Simple Pendulum Oscillations |
|---|---|---|
| Restoring Force | Spring-Mass: $F = -kx$ (proportional to displacement) | Simple Pendulum: $F = -mgsin heta approx -mg heta = -(mg/L)x$ (proportional to displacement for small angles) |
| Period Formula | Spring-Mass: $T = 2pisqrt{m/k}$ | Simple Pendulum: $T = 2pisqrt{L/g}$ (for small angles) |
| Dependence on Mass | Spring-Mass: Period depends on mass (T increases with m) | Simple Pendulum: Period is independent of mass (for small angles) |
| Dependence on Gravity | Spring-Mass: Period is independent of 'g' (for horizontal oscillation; for vertical, 'g' shifts equilibrium but not period) | Simple Pendulum: Period depends on 'g' (T decreases with increasing g) |
| Energy Transformation | Spring-Mass: Kinetic energy $leftrightarrow$ Elastic potential energy | Simple Pendulum: Kinetic energy $leftrightarrow$ Gravitational potential energy |