A second-order linear hyperbolic partial differential equation that governs the propagation of various types of waves. In its simplest form, it is written as \(\frac{\partial^2 u}{\partial t^2} = c^2 \nabla^2 u\), where \(u(\vec{x},t)\) is the amplitude of the wave, \(c\) is the wave speed, and \(\nabla^2\) is the Laplace operator. It models phenomena like vibrating strings, sound waves, and light waves.
The Wave Equation (physics)
- Jean le Rond d’Alembert
The wave equation is the archetypal hyperbolic PDE. Unlike the heat equation, it is second-order in time, which gives rise to its oscillatory, wave-like solutions. The presence of the \(\frac{\partial^2 u}{\partial t^2}\) term implies that acceleration is proportional to the local curvature of the function, a relationship characteristic of restorative forces like tension in a string. The constant \(c\) represents the finite speed at which disturbances propagate through the medium.
A crucial feature of the wave equation is the principle of causality and finite propagation speed. A disturbance at a point \(\vec{x}_0\) at time \(t_0\) can only affect points \(\vec{x}\) at a later time \(t\) that are within a distance of \(c(t-t_0)\). This region is known as the ‘cone of influence’. Conversely, the value of the solution at \((\vec{x}, t)\) depends only on the initial data within its ‘domain of dependence’. This contrasts sharply with the infinite propagation speed of the heat equation.
In one spatial dimension, the equation \(u_{tt} = c^2 u_{xx}\) has a remarkably simple general solution, discovered by d’Alembert: \(u(x,t) = F(x-ct) + G(x+ct)\). This represents the superposition of two waves traveling in opposite directions with speed \(c\). The shapes of these waves, determined by the functions \(F\) and \(G\), are preserved as they propagate.
Type
Disruption
Usage
Precursors
- newton’s laws of motion
- hooke’s law for elastic forces
- development of calculus and partial derivatives
- studies of vibrating strings by brook taylor and johann bernoulli
Applications
- acoustics and audio engineering
- electromagnetism (propagation of light and radio waves)
- seismology for modeling earthquakes
- fluid dynamics for surface waves
- general relativity for gravitational waves
Patents:
Potential Innovations Ideas
Professionals (100% free) Membership Required
You must be a Professionals (100% free) member to access this content.
AVAILABLE FOR NEW CHALLENGES
Mechanical Engineer, Project or R&D Manager
Available for a new challenge on short notice.
Contact me on LinkedIn
Plastic metal electronics integration, Design-to-cost, GMP, Ergonomics, Medium to high-volume devices & consumables, Regulated industries, CE & FDA, CAD, Solidworks, Lean Sigma Black Belt, medical ISO 13485
We are looking for a new sponsor
Your company or institution is into technique, science or research ?
> send us a message <
Receive all new articles
Free, no spam, email not distributed nor resold
or you can get your full membership -for free- to access all restricted content >here<
Historical Context
The Wave Equation (physics)
(if date is unknown or not relevant, e.g. "fluid mechanics", a rounded estimation of its notable emergence is provided)
Related Invention, Innovation & Technical Principles