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JГјrgen Jost - Partial Differential Equations

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JГјrgen Jost Partial Differential Equations
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    Partial Differential Equations
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Springer Science+Business Media New York 2013
Jrgen Jost Partial Differential Equations Graduate Texts in Mathematics 10.1007/978-1-4614-4809-9_1
1. Introduction: What Are Partial Differential Equations?
Jrgen Jost 1
(1)
Max Planck Institute for Mathematics in the Sciences, Leipzig, Germany
As a first answer to the question, What are PDEs, we would like to give a definition:
Definition 1.
A PDE is an equation involving derivatives of an unknown function Picture 1 , where is an open subset of Partial Differential Equations - image 2 , d 2 (or, more generally, of a differentiable manifold of dimension d 2).
Often, one also considers systems of PDEs for vector-valued functions Partial Differential Equations - image 3 , or for mappings with values in a differentiable manifold.
The preceding definition, however, is misleading, since in the theory of PDEs one does not study arbitrary equations but concentrates instead on those equations that naturally occur in various applications (physics and other sciences, engineering, economics) or in other mathematical contexts.
Thus, as a second answer to the question posed in the title, we would like to describe some typical examples of PDEs. We shall need a little bit of notation: A partial derivative will be denoted by a subscript,
Partial Differential Equations - image 4
In case d =2, we write x , y in place of Partial Differential Equations - image 5 . Otherwise, x is the vector Partial Differential Equations - image 6 .
Examples.
  1. (1)
    The Laplace equation
    or more generally the Poisson equation For example the real and imaginary - photo 7
    or, more generally, the Poisson equation
    For example the real and imaginary parts u and v of a holomorphic function - photo 8
    For example, the real and imaginary parts u and v of a holomorphic function open satisfy the Laplace equation This easily follows from the - photo 9 ( open satisfy the Laplace equation This easily follows from the CauchyRiemann - photo 10 open) satisfy the Laplace equation. This easily follows from the CauchyRiemann equations:
    implies The CauchyRiemann equations themselves represent a system of PDEs The - photo 11
    implies
    The CauchyRiemann equations themselves represent a system of PDEs The Laplace - photo 12
    The CauchyRiemann equations themselves represent a system of PDEs. The Laplace equation also models many equilibrium states in physics, and the Poisson equation is important in electrostatics.
  2. (2)
    The heat equation: Here, one coordinate t is distinguished as the time coordinate, while the remaining coordinates represent spatial variables We consider and pose the equation The heat - photo 13 represent spatial variables. We consider
    and pose the equation The heat equation models heat and other diffusion - photo 14
    and pose the equation
    The heat equation models heat and other diffusion processes 3 The wave - photo 15
    The heat equation models heat and other diffusion processes.
  3. (3)
    The wave equation: With the same notation as in (2), here we have the equation
    Partial Differential Equations - image 16
    It models wave and oscillation phenomena.
  4. (4)
    The Kortewegde Vries equation
    Partial Differential Equations - image 17
    (notation as in (2), but with only one spatial coordinate x ) models the propagation of waves in shallow waters.
  5. (5)
    The MongeAmpre equation
    Partial Differential Equations - image 18
    or in higher dimensions
    Partial Differential Equations - image 19
    with a given function f , is used for finding surfaces (or hypersurfaces) with prescribed curvature.
  6. (6)
    The minimal surface equation
    Partial Differential Equations - image 20
    describes an important class of surfaces in Partial Differential Equations - image 21 .
  7. (7)
    The Maxwell equations for the electric field strength Partial Differential Equations - image 22 and the magnetic field strength Partial Differential Equations - image 23 as functions of Partial Differential Equations - image 24 :
    Partial Differential Equations - image 25
    where div and curl are the standard differential operators from vector analysis with respect to the variables Partial Differential Equations - image 26 .
  8. (8)
    The NavierStokes equations for the velocity v ( x , t ) and the pressure p ( x , t ) of an incompressible fluid of density Partial Differential Equations - image 27 and viscosity :
    Partial Differential Equations - image 28
    (0)
    ( d =3, Partial Differential Equations - image 29 ).
  9. (9)
    The Einstein field equations of the theory of general relativity for the curvature of the metric ( g ij ) of space-time:
    Here is a constant T ij is the energymomentum tensor considered as given - photo 30
    Here, is a constant, T ij is the energymomentum tensor (considered as given), while
    with and and Thu - photo 31
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