Heat equation
The heat equation is an important partial differential equation which describes the variation of temperature in a given region over time. In the special case of heat propagation in an isotropic and homogeneous medium in the 3-dimensional space, this equation is
Related Topics:
Partial differential equation - Isotropic - Homogeneous - Dimension
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:u_t = k ( u_{xx} + u_{yy} + u_{zz} ) quad
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where:
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- u(t, x, y, z) is temperature as a function of time and space;
- ut is the rate of change of temperature at a point over time;
- , , and are the second spatial derivatives (thermal conductions) of temperature in the x, y, and z directions, respectively
- k is a material-specific constant called thermal diffusivity.
The heat equation is a consequence of Fourier's law of cooling (see heat conduction).
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To solve the heat equation, we also need to specify boundary conditions for u.
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Solutions of the heat equation are characterized by a gradual smoothing of the initial temperature distribution by the flow of heat from warmer to colder areas of an object.
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The heat equation is the prototypical example of a parabolic partial differential equation.
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Using the Laplace operator, the heat equation can be generalized to
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:u_t = k Delta u, quad
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where the Laplace operator is taken in the spatial variables.
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The heat equation also describes other physical processes, such as diffusion. It also can be used to model some processes in finance.
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~ Table of Content ~
| ► | Introduction |
| ► | Solving the heat equation using Fourier series |
| ► | Heat conduction in non-homogeneous anisotropic media |
| ► | Applications |
| ► | References |
| ► | External links |
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