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You might think that as long as we specify an infinitely smooth heat
flux, this problem would not arise. And indeed, for some (not all)
infinitely smooth heat fluxes, there is in theory a solution to the
initial value problem for the Laplace equation. The difficulty is
that if we make even the slightest, imperceptible kink in such a heat
flux distribution, it is singular and the solution suddenly no longer
exists. As a result, even the smallest change in the given conditions
can completely alter the solution. A unique solution would still
require infinite precision in the values of the heat flux.
A problem in which small disturbances can have arbitrarily large
effects is called an improperly posed problem. Both the initial
value problem for the Laplace equation and the boundary value problem
for the wave equation are improperly posed. So is the problem
of trying to solve the heat equation backward in time, for similar
reasons: since the heat equation smooths singularities,
no earlier time solution can give rise to a singularity
in the bar at the later starting time.
On the other hand, it is perfectly well possible to solve the wave equation
backward in time.
Next: About the numerical
Up: The Laplace equation.
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