(mathematics) An equation where the unknown function occurs under an integral sign.
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(mathematics) An equation where the unknown function occurs under an integral sign.
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where f(x) is known and j(t) is to be found, given certain conditions on f. Such equations are useful in solving differential equations.For more information on integral equation, visit Britannica.com.
| Wikipedia: Integral equation |
In mathematics, an integral equation is an equation in which an unknown function appears under an integral sign. There is a close connection between differential and integral equations, and some problems may be formulated either way. See, for example, Maxwell's equations.
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The most basic type of integral equation is a Fredholm equation of the first type:

The notation follows Arfken. Here φ is an unknown function, f is a known function, and K is another known function of two variables, often called the kernel function. Note that the limits of integration are constant; this is what characterizes a Fredholm equation.
If the unknown function occurs both inside and outside of the integral, it is known as a Fredholm equation of the second type:

The parameter λ is an unknown factor, which plays the same role as the eigenvalue in linear algebra.
If one limit of integration is variable, it is called a Volterra equation. Thus Volterra equations of the first and second types, respectively, would appear as:


In all of the above, if the known function f is identically zero, it is called a homogeneous integral equation. If f is nonzero, it is called an inhomogeneous integral equation.
Integral equations are classified according to three different dichotomies, creating eight different kinds:
Integral equations are important in many applications. Problems in which integral equations are encountered include radiative energy transfer and the oscillation of a string, membrane, or axle. Oscillation problems may also be solved as differential equations.
Both Fredholm and Volterra equations are linear integral equations, due to the linear behaviour of φ(x) under the integral. A nonlinear Volterra integral equation has the general form:
,where F is a known function.
Certain homogeneous linear integral equations can be viewed as the continuum limit of eigenvalue equations. Using index notation, an eigenvalue equation can be written as
,where
is a matrix,
is one of its eigenvectors, and λ is the associated eigenvalue.
Taking the continuum limit, by replacing the discrete indices i and j with continuous variables x and y, gives
,where the sum over j has been replaced by an integral over y and the matrix Mi,j and vector vi have been replaced by the 'kernel' K(x,y) and the eigenfunction
. (The limits on the integral are fixed, analogously to the limits on the sum over j.) This gives a linear homogeneous Fredholm equation of the second type.
In general, K(x,y) can be a distribution, rather than a function in the strict sense. If the distribution K has support only at the point x = y, then the integral equation reduces to a differential eigenfunction equation.
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| Best of the Web: Integral equation |
Some good "Integral equation" pages on the web:
Math mathworld.wolfram.com |
| homogeneous integral equation (mathematics) | |
| Hermitian kernel (mathematics) | |
| Hilbert-Schmidt theory (mathematics) |
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