Hyperbolic partial differential equation

In mathematics, a hyperbolic partial differential equation of order n is a partial differential equation (PDE) that, roughly speaking, has a well-posed initial value problem for the first n−1 derivatives. More precisely, the Cauchy problem can be locally solved for arbitrary initial data along any non-characteristic hypersurface. Many of the equations of mechanics are hyperbolic, and so the study of hyperbolic equations is of substantial contemporary interest. The model hyperbolic equation is the wave equation. In one spatial dimension, this is

$u_{tt} - u_{xx} = 0.\,$

The equation has the property that, if u and its first time derivative are arbitrarily specified initial data on the initial line t = 0 (with sufficient smoothness properties), then there exists a solution for all time.

The solutions of hyperbolic equations are "wave-like." If a disturbance is made in the initial data of a hyperbolic differential equation, then not every point of space feels the disturbance at once. Relative to a fixed time coordinate, disturbances have a finite propagation speed. They travel along the characteristics of the equation. This feature qualitatively distinguishes hyperbolic equations from elliptic partial differential equations and parabolic partial differential equations. A perturbation of the initial (or boundary) data of an elliptic or parabolic equation is felt at once by essentially all points in the domain.

Although the definition of hyperbolicity is fundamentally a qualitative one, there are precise criteria that depend on the particular kind of differential equation under consideration. There is a well-developed theory for linear differential operators, due to Lars Gårding, in the context of microlocal analysis. Nonlinear differential equations are hyperbolic if their linearizations are hyperbolic in the sense of Gårding. There is a somewhat different theory for first order systems of equations coming from systems of conservation laws.

1 Definition
2 Examples
3 Hyperbolic system of partial differential equations
4 Hyperbolic system and conservation laws
5 See also
6 Bibliography
7 External links

Definition

A partial differential equation is hyperbolic at a point P provided that the Cauchy problem is uniquely solvable in a neighborhood of P for any initial data given on a non-characteristic hypersurface passing through P. Here the prescribed initial data consists of all (transverse) derivatives of the function on the surface up to one less than the order of the differential equation.

Examples

By a linear change of variables, any equation of the form

$Au_{xx} + Bu_{xy} + Cu_{yy} + \text{(lower order terms)} = 0 \,$

with

$B^2 - 4 A C > 0 \,$

can be transformed to the wave equation, apart from lower order terms which are inessential for the qualitative understanding of the equation. This definition is analogous to the definition of a planar hyperbola.

The one-dimensional wave equation:

$\frac{\partial^2 u}{\partial t^2} - c^2\frac{\partial^2 u}{\partial x^2} = 0$

is an example of a hyperbolic equation. The two-dimensional and three-dimensional wave equations also fall into the category of hyperbolic PDE.

This type of second-order hyperbolic partial differential equation may be transformed to a hyperbolic system of first-order differential equations.

Hyperbolic system of partial differential equations

Consider the following system of $s$ first order partial differential equations for $s$ unknown functions $\vec u = (u_1, \ldots, u_s)$ , $\vec u =\vec u (\vec x,t)$ , where $\vec x \in \mathbb{R}^d$

$(*) \quad \frac{\partial \vec u}{\partial t} + \sum_{j=1}^d \frac{\partial}{\partial x_j} \vec {f^j} (\vec u) = 0,$

$\vec {f^j} \in C^1(\mathbb{R}^s, \mathbb{R}^s), j = 1, \ldots, d$ are once continuously differentiable functions, nonlinear in general.

Now define for each $\vec {f^j}$ a matrix $s \times s$

$A^j:= \begin{pmatrix} \frac{\partial f_1^j}{\partial u_1} & \cdots & \frac{\partial f_1^j}{\partial u_s} \\ \vdots & \ddots & \vdots \\ \frac{\partial f_s^j}{\partial u_1} & \cdots & \frac{\partial f_s^j}{\partial u_s} \end{pmatrix} ,\text{ for }j = 1, \ldots, d.$

We say that the system $( * )$ is hyperbolic if for all $\alpha_1, \ldots, \alpha_d \in \mathbb{R}$ the matrix $A := \alpha_1 A^1 + \cdots + \alpha_d A^d$ has only real eigenvalues and is diagonalizable.

If the matrix $A$ has distinct real eigenvalues, it follows that it's diagonalizable. In this case the system $( * )$ is called strictly hyperbolic.

Hyperbolic system and conservation laws

There is a connection between a hyperbolic system and a conservation law. Consider a hyperbolic system of one partial differential equation for one unknown function $u = u(\vec x, t)$ . Then the system $( * )$ has the form

$(**) \quad \frac{\partial u}{\partial t} + \sum_{j=1}^d \frac{\partial}{\partial x_j} {f^j} (u) = 0,$

Now $u$ can be some quantity with a flux $\vec f = (f^1, \ldots, f^d)$ . To show that this quantity is conserved, integrate $( * * )$ over a domain $Ω$

$\int_{\Omega} \frac{\partial u}{\partial t} d\Omega + \int_{\Omega} \nabla \cdot \vec f(u) d\Omega = 0.$

If $u$ and $\vec f$ are sufficiently smooth functions, we can use the divergence theorem and change the order of the integration and $\partial / \partial t$ to get a conservation law for the quantity $u$ in the general form

$\frac{d}{dt} \int_{\Omega} u d\Omega + \int_{\Gamma} \vec f(u) \cdot \vec n d\Gamma = 0,$

which means that the time rate of change of $u$ in the domain $Ω$ is equal to the net flux of $u$ through its boundary $Γ$ . Since this is an equality, it can be concluded that $u$ is conserved within $Ω$ .

Bibliography

Evans, Lawrence C. (2010) [1998], Partial differential equations, Graduate Studies in Mathematics, 19 (2nd ed.), Providence, R.I.: American Mathematical Society, MR 2597943, ISBN 978-0-8218-4974-3, http://www.ams.org/journals/bull/2000-37-03/S0273-0979-00-00868-5/S0273-0979-00-00868-5.pdf
A. D. Polyanin, Handbook of Linear Partial Differential Equations for Engineers and Scientists, Chapman & Hall/CRC Press, Boca Raton, 2002. ISBN 1-58488-299-9 [Amazon-US | Amazon-UK]
Rozhdestvenskii, B.L. (2001), "Hyperbolic partial differential equation", in Hazewinkel, Michiel, Encyclopaedia of Mathematics, Springer, ISBN 978-1556080104, http://eom.springer.de/H/h048300.htm

External links

Linear Hyperbolic Equations at EqWorld: The World of Mathematical Equations.
Nonlinear Hyperbolic Equations at EqWorld: The World of Mathematical Equations.

Open source encyclopedia content modification information:

Authorship and Review

Open source encyclopedia content provided here is not reviewed directly by PediaView.com. Content is authored by an open community of volunteers and is not produced by or in any way affiliated with PediaView.com.

Usage Guidelines

This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article on "Hyperbolic partial differential equation", which is available in its original form here:

http://en.wikipedia.org/w/index.php?title=Hyperbolic_partial_differential_equation

All Wikipedia text is available under the terms of the GNU Free Documentation License. Wikipedia® itself is a registered trademark of the Wikimedia Foundation, Inc.