Neumann boundary condition

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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, the condition specifies the values in which the derivative of a solution is applied within the boundary of the domain.

It is possible to describe the problem using other boundary conditions: a Dirichlet boundary condition specifies the values of the solution itself (as opposed to its derivative) on the boundary, whereas the Cauchy boundary condition, mixed boundary condition and Robin boundary condition are all different types of combinations of the Neumann and Dirichlet boundary conditions.

Examples[edit]

Ordinary differential equation[edit]

For an ordinary differential equation, for instance,

the Neumann boundary conditions on the interval take the form

where and are given numbers.

Partial differential equation[edit]

For a partial differential equation, for instance,

where denotes the Laplace operator, the Neumann boundary conditions on a domain take the form

where denotes the (typically exterior) normal to the boundary , and f is a given scalar function.

The normal derivative, which shows up on the left side, is defined as

where is the gradient (vector) and the dot is the inner product.

It becomes clear that the boundary must be sufficiently smooth such that the normal derivative can exist, since for example at corner points of the boundary the normal vector is not well defined.

Applications[edit]

The following engineering applications involve the use of Neumann boundary conditions:

  • In thermodynamics, a prescribed heat flux from a surface would serve as boundary condition. For example, a perfect insulator would have no flux while an electrical component may be dissipating at a known power.

See also[edit]

References[edit]

  1. ^ Cheng, A. H.-D.; Cheng, D. T. (2005). "Heritage and early history of the boundary element method". Engineering Analysis with Boundary Elements. 29 (3): 268. doi:10.1016/j.enganabound.2004.12.001.