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Burgers' equation

Burgers' equation is a fundamental partial differential equation from fluid mechanics. It occurs in various areas of applied mathematics, such as modelling of gas dynamics and traffic flow . It is named for Johannes Martinus Burgers (1895-1981).

The general form of Burgers' equation is:

\frac{\partial u}{\partial t} + u \frac{\partial u}{\partial x} = \mu \frac{\partial^2 u}{\partial x^2}.

Here μ > 0 is a viscosity coefficient. When μ = 0, Burgers' equation becomes the inviscid Burgers' equation:

\frac{\partial u}{\partial t} + u \frac{\partial u}{\partial x} = 0,

which is a prototype for equations for which the solution can develop discontinuities (shock waves).

Solution

The inviscid Burgers' equation is a first order partial differential equation. Its solution can be constructed by the method of characteristics. This method yields that if X(t) is a solution of the ordinary differential equation

dX(t) / dt = u(X(t),t)

then U(t): = u(X(t),t) is constant as a function of t. Hence (X(t),U(t)) is a solution of the system of ordinary equations

dX / dt = U
dU / dt = 0.

The solutions of this system are given in terms of the initial values by

X(t) = X(0) + tU(0)
U(t) = U(0).

Substitute X(0) = η, then U(0) = u(X(0),0) = u(η,0). Now the system becomes

X(t) = η + tu(η,0)
U(t) = U(0).

Conclusion:

u(η,0) = U(0) = U(t) = u(X(t),t) = u(η + tu(η,0),t).

This is an implicit relation that determines the solution of the inviscid Burgers' equation.

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Last updated: 06-01-2005 20:13:39
10-26-2009 08:16:03
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