Category:Parabolic: Difference between revisions
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A second order linear partial differential equation can be written as | A second order linear partial differential equation can be written as | ||
<math>\sum^n_{i,j=1} a_{ij} \frac{\partial^2u}{\partial x_i \partial x_j} +\ | <math>\sum^n_{i,j=1} a_{ij} \frac{\partial^2u}{\partial x_i \partial x_j} +\, \text{lower-order terms} = 0</math>. | ||
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If <math>A=(a_{ij})_{ij}</math> is positive or negative semidefinite with exact one eigenvalue zero, the partial differential equation is called parabolic. | If the matrix <math>A=(a_{ij})_{ij}</math> is positive or negative semidefinite with exact one eigenvalue zero, the partial differential equation is called parabolic. | ||
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An example is the heat equation: <math>\frac{\partial u}{\partial t}-\Delta u = f</math>, | An example is the heat equation: <math>\frac{\partial u}{\partial t}-\Delta u = f</math>, | ||
where <math>\Delta</math> denotes the Laplace operator, <math>u</math> is the unknown, and the function <math>f</math> is given. | where <math>\Delta</math> denotes the Laplace operator, <math>u</math> is the unknown, and the function <math>f</math> is given. | ||
Latest revision as of 15:21, 24 February 2016
This category contains all control problems which are governed by a parabolic partial differential equation.
A second order linear partial differential equation can be written as .
If the matrix is positive or negative semidefinite with exact one eigenvalue zero, the partial differential equation is called parabolic.
An example is the heat equation: , where denotes the Laplace operator, is the unknown, and the function is given.
Pages in category "Parabolic"
This category contains only the following page.