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SimplePendulum&HarmonicMotion

Explore harmonic motion and large-angle pendulum physics. Adjust string length, bob mass, release angle, and air damping to visualize phase-space trajectories and measure exact oscillation periods.

Simple Pendulum & Harmonic Motion interactive Physics simulation illustration
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Interactive Experiment Guide

Use this studio like a real-time physics workbench

Start with fundamental scientific principles, launch the simulation, and verify mathematical predictions against real-time outcomes.

DisciplinePhysics
Simulation ModeInteractive Numeric Engine
Governing ModelRunge-Kutta RK4 Non-Linear Oscillator
DeploymentIn-Browser WebAssembly / GPU
01

Scientific Foundation

What is simple pendulum & harmonic motion?

A simple pendulum consists of a point mass m suspended on a massless string of length L. The exact non-linear equation of motion is d²θ/dt² = -(g/L) sin θ - γ(dθ/dt). For small angles (θ ≤ 15°), sin θ ≈ θ yields Simple Harmonic Motion with period T0 = 2π√(L/g). For larger angles, exact elliptic integrals demonstrate period elongation T ≈ T0(1 + ¼sin²(θ0/2)).

02

Interactive Simulation Flow

Experiment Execution & Governing Equations

Launch the simulation workspace, adjust parameters in real time, and observe the immediate response in the telemetry and graphical indicator loops.

Small-Angle Approximation & Large-Angle CorrectionT_0 = 2\pi\sqrt{\frac{L}{g}} \quad \text{and} \quad T \approx T_0\left(1 + \frac{1}{4}\sin^2\frac{\theta_0}{2}\right)

Frequently Asked Questions

Simple Pendulum & Harmonic Motion FAQ

4 Answers

Because gravitational force (which accelerates the bob) and inertia (which resists acceleration) are both directly proportional to mass m. In the equation of motion md²θ/dt² = -mg sin θ, mass cancels out completely on both sides, leaving d²θ/dt² = -(g/L) sin θ.

Knowledge Graph & Related Concepts