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Goursat Problem


For the hyperbolic partial differential equation

u_(xy)=F(x,y,u,p,q)
(1)
p=u_x
(2)
q=u_y
(3)

on a domain Omega, Goursat's problem asks to find a solution u(x,y) of (3) from the boundary conditions

u(0,t)=phi(t)
(4)
u(t,1)=psi(t)
(5)
phi(1)=phi(0)
(6)

for 0<=t<=1 that is regular in Omega and continuous in the closure Omega^_, where phi and psi are specified continuously differentiable functions.

The linear Goursat problem corresponds to the solution of the equation

 L^~u=u_(xy)+au_x+bu_y+cu=f,
(7)

which can be effected using the so-called Riemann function R(x,y;xi,eta). The use of the Riemann function to solve the linear Goursat problem is called the Riemann method.


See also

Boundary Value Problem, Hyperbolic Partial Differential Equation, Function, Riemann Method

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References

Courant, R. and Hilbert, D. Methods of Mathematical Physics, Vol. 2. New York: Wiley, 1989.Goursat, E. A Course in Mathematical Analysis, Vol. 3: Variation of Solutions and Partial Differential Equations of the Second Order & Integral Equations and Calculus of Variations Paris: Gauthier-Villars, 1923.Hazewinkel, M. (Managing Ed.). Encyclopaedia of Mathematics: An Updated and Annotated Translation of the Soviet "Mathematical Encyclopaedia." Dordrecht, Netherlands: Reidel, p. 289, 1988.Tricomi, F. G. Integral Equations. New York: Interscience, 1957.

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Goursat Problem

Cite this as:

Weisstein, Eric W. "Goursat Problem." From MathWorld--A Wolfram Web Resource. https://mathworld.wolfram.com/GoursatProblem.html

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