Laplace's equation
Laplace's equation is a second-order partial differential equation named after the French mathematician Pierre-Simon Laplace. It is a fundamental equation in the field of potential theory and appears in many areas of physics and engineering, particularly in the study of electrostatics, gravitation, and fluid dynamics.
Mathematical Formulation[edit | edit source]
Laplace's equation is given by: \[ \Delta \phi = 0 \] where \( \Delta \) is the Laplace operator (or Laplacian) and \( \phi \) is a twice-differentiable function. In three-dimensional Cartesian coordinates, the Laplace operator is expressed as: \[ \Delta \phi = \frac{\partial^2 \phi}{\partial x^2} + \frac{\partial^2 \phi}{\partial y^2} + \frac{\partial^2 \phi}{\partial z^2} \]
Applications[edit | edit source]
Laplace's equation is widely used in various fields:
- In electrostatics, it describes the potential field generated by a distribution of electric charges in the absence of free charges.
- In fluid dynamics, it is used to describe the velocity potential of an incompressible and irrotational fluid flow.
- In gravitation, it describes the gravitational potential in a region with no mass.
Boundary Conditions[edit | edit source]
Solutions to Laplace's equation are determined by the boundary conditions of the problem. Common types of boundary conditions include:
- Dirichlet boundary condition: Specifies the value of the function \( \phi \) on the boundary.
- Neumann boundary condition: Specifies the value of the normal derivative of \( \phi \) on the boundary.
- Robin boundary condition: A combination of Dirichlet and Neumann boundary conditions.
Harmonic Functions[edit | edit source]
A function that satisfies Laplace's equation is called a harmonic function. Harmonic functions have several important properties:
- They are infinitely differentiable within the domain.
- They satisfy the mean value property.
- They exhibit the maximum principle, meaning that the maximum and minimum values of a harmonic function occur on the boundary of the domain.
Related Equations[edit | edit source]
Laplace's equation is a special case of the more general Poisson's equation, which is given by: \[ \Delta \phi = f \] where \( f \) is a known function. When \( f = 0 \), Poisson's equation reduces to Laplace's equation.
See Also[edit | edit source]
- Poisson's equation
- Harmonic function
- Laplace operator
- Dirichlet problem
- Neumann problem
- Potential theory
References[edit | edit source]
External Links[edit | edit source]
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