The simple pendulum is a perfect example of a second-order differential equation in action. The motion of a pendulum demonstrates how acceleration, velocity, and position are interrelated through a beautiful mathematical relationship.
Adjust these parameters to see how they affect the pendulum's motion:
A pendulum's motion is described by a second-order differential equation:
$$\frac{d^2\theta}{dt^2} + \frac{b}{m}\frac{d\theta}{dt} + \frac{g}{L}\sin(\theta) = 0$$This equation emerges from:
This gives us the simplified equation:
$$\frac{d^2\theta}{dt^2} + \frac{b}{m}\frac{d\theta}{dt} + \frac{g}{L}\theta = 0$$Where:
In an ideal pendulum (no damping), the total energy constantly switches between: - Potential energy at the highest points - Kinetic energy at the lowest point This conservation creates the periodic motion we observe.
When forced at its natural frequency (ω = √(g/L)), a pendulum exhibits resonance, dramatically increasing its amplitude. This principle is crucial in many engineering applications and natural phenomena.