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 of the derivative applied at 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.
For an ordinary differential equation, for instance,
y''+y=0,
the Neumann boundary conditions on the interval take the form
y'(a)=\alpha, y'(b)=\beta,
where and are given numbers.
For a partial differential equation, for instance,
\nabla2y+y=0,
where denotes the Laplace operator, the Neumann boundary conditions on a domain take the form
| \partialy | |
| \partialn |
(x)=f(x) \forallx\in\partial\Omega,
where denotes the (typically exterior) normal to the boundary, and is a given scalar function.
The normal derivative, which shows up on the left side, is defined as
| \partialy | |
| \partialn |
(x)=\nablay(x) ⋅ \hat{n
where represents the gradient vector of, is the unit normal, and represents the inner product operator.
It becomes clear that the boundary must be sufficiently smooth such that the normal derivative can exist, since, for example, at corner points on the boundary the normal vector is not well defined.
The following applications involve the use of Neumann boundary conditions: