Hyperbolic Equations: Definition & Explanation

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SUMMARY

The equation (d²u/dt²) - (Δu) = 0 is classified as a hyperbolic equation, characterized by its two characteristic lines used for solving the equation. This classification is based on the analogy with the hyperbola defined by x² - y² = 1. In contrast, the heat equation, represented as ∂u/∂t = ∂²u/∂x², is a parabolic equation with a single characteristic line, while Laplace's equation, ∂²u/∂x² + ∂²u/∂y² = 0, is classified as elliptic due to the absence of characteristic lines.

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(d2^u/dt^2) - (delta u) = 0 is called a hyperbolic equation.

Why is this? What makes an equation a hyperbolic equation?
 
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The partial differential equation
[tex]\frac{\partial^2u}{\partial t^2}= \frac{\partial^2 u}{\partial x^2}[/tex]
and its extension to 2 or 3 space dimensions, is called "hyperbolic" in an obvious analogy with the hyperbolic equation
[tex]x^2- y^2= 1[/tex]
In addition, just as the hyperbola has two asymptotes, so the hyperbolic differential equation has two "characteristic" lines that can be used to solve the equation.

The heat (or diffusion) equation,
[tex]\frac{\partial u}{\partial t}= \frac{\partial u^2}{\partial x^2}[/tex]
has only a single characteristic line and is a "parabolic" equation.

Laplace's equation,
[tex]\frac{\partial^2 u}{\partial x^2}+ \frac{\partial^2 u}{\partial y^2}= 0[/tex]
has no characteristic lines and is an "elliptic" equation.
 

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