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Initial Value Problems of Hyperbolic Type



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The wave equation,
 equation1116
is the prototype for PDE's of hyperbolic type. We study the pure initial-value problem associated with (hyper.1), augmented with 2tex2html_wrap_inline10969-periodic boundary conditions and subject to prescribed initial conditions,
 equation1118
We can solve this equation using the method of characteristics, which yields
 equation1120
We shall study the manner in which the solution depends on the initial data. In this context the following features are of importance.  

  1. : the principle of superposition holds.
  2. : influence propagates with speed tex2html_wrap_inline10971 a. This is the essential feature of hyperbolicity. In the wave equation it is reflected by the fact that the value of w at (x,t) is not influenced by initial values outside domain of dependence (x - at, x + at).
  3. for large enough set of admissible initial data: arbitrary tex2html_wrap_inline10979 initial data can be prescribed and the corresponding solution is tex2html_wrap_inline10979.
  4. : the solution is uniquely determined for tex2html_wrap_inline10983 by its initial data.
  5. . The wave equation (hyper.1) describes the motion of a string with kinetic energy, tex2html_wrap_inline10985, and potential one, tex2html_wrap_inline10987. In order to show that the total energy
    displaymath1122
    is conserved in time we may proceed in one of two ways: either by the so called energy method or by Fourier analysis.




Eitan Tadmor
Thu Jan 22 19:07:34 PST 1998