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Parabolic Equations

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ℓ Goes to Plus Infinity

Part of the book series: Birkhäuser Advanced Texts ((BAT))

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Abstract

The problems we shall solve now are of the so-called heat equation type. Such theory is available in many places (see for instance [21], [2], [6], [17], [8]) but for the self-completeness of this book we would like to recall the main ideas. Φ being a domain of ℝ n , we would like, for instance, to find a function u(x, t) such that

$$\left\{ \begin{gathered} {u_t} - \Delta u = f in \Omega \times (0,T), \hfill \\ u(x,t) = 0 on \Gamma \times (0,T), \hfill \\ u(x,0) = {u_0}(x) on \Omega , \hfill \\ \end{gathered} \right.$$
(8.1)

f(x,t), u 0(x) are two given data. Clearly, the second equation of (8.1) can also be interpreted as

$$ u( \cdot ,t) \in H_0^1\left( \Omega \right). $$
(8.2)

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© 2002 Springer Basel AG

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Chipot, M. (2002). Parabolic Equations. In: ℓ Goes to Plus Infinity. Birkhäuser Advanced Texts. Birkhäuser, Basel. https://doi.org/10.1007/978-3-0348-8173-9_8

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  • DOI: https://doi.org/10.1007/978-3-0348-8173-9_8

  • Publisher Name: Birkhäuser, Basel

  • Print ISBN: 978-3-0348-9465-4

  • Online ISBN: 978-3-0348-8173-9

  • eBook Packages: Springer Book Archive

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