Difference between revisions of "Category:Hyperbolic"

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This category contains all control problems which are governed by a hyperbolic partial differential equation.  
 
This category contains all control problems which are governed by a hyperbolic partial differential equation.  
 
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<p>
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A second order linear partial differential equation can be written as
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<math>\sum^n_{i,j=1} a_{ij} \frac{\partial^2u}{\partial x_i \partial x_j} +\quad \textrm{ lower-order terms} = 0</math>.
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If <math>A=(a_{ij})_{ij}</math> is indefinite such that <math>n-1</math> eigenvalues have the same sign and the remaining eigenvalue the other sign, the partial differential equation is called hyperbolic.
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An example is the wave equation: <math>\frac{\partial^2 u}{\partial t^2}-\Delta u = f</math>,
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where <math>\Delta</math> denotes the Laplace operator, <math>u</math> is the unknown, and the function <math>f</math> given.
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</p>
  
 
<!--List of all categories this page is part of. List characterization of solution behavior, model properties, ore presence of implementation details (e.g., AMPL for AMPL model) here -->
 
<!--List of all categories this page is part of. List characterization of solution behavior, model properties, ore presence of implementation details (e.g., AMPL for AMPL model) here -->

Revision as of 15:29, 24 February 2016

This category contains all control problems which are governed by a hyperbolic partial differential equation.

A second order linear partial differential equation can be written as \sum^n_{i,j=1} a_{ij} \frac{\partial^2u}{\partial x_i \partial x_j} +\quad \textrm{ lower-order terms} = 0. If A=(a_{ij})_{ij} is indefinite such that n-1 eigenvalues have the same sign and the remaining eigenvalue the other sign, the partial differential equation is called hyperbolic. An example is the wave equation: \frac{\partial^2 u}{\partial t^2}-\Delta u = f, where \Delta denotes the Laplace operator, u is the unknown, and the function f given.

Pages in category "Hyperbolic"

This category contains only the following page.