(mathematics) The boundary condition imposed on the Neumann problem in potential theory.
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(mathematics) The boundary condition imposed on the Neumann problem in potential theory.
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In mathematics, the Neumann (or second-type) boundary condition is a type of boundary condition, named after Carl Neumann[1]. When imposed on an ordinary or a partial differential equation, it specifies the values that the derivative of a solution is to take on the boundary of the domain.
In the case of an ordinary differential equation, for example such as:

on the interval [0,1] the Neumann boundary conditions take the form:


where α₁ and α₂ are given numbers.
For a partial differential equation on a domain Ω⊂ℝⁿ such as:

where ∇² denotes the Laplacian, the Neumann boundary condition takes the form:

Here, n denotes the (typically exterior) normal to the boundary ∂Ω and f is a given scalar function. The normal derivative which shows up on the left-hand side is defined as :

where ∇ is the gradient and the dot is the inner product.
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