## A word on PDEs

April 2, 2011 by micropore

So far, we discussed very simple problems. From now one, we want to simulate some simple problems, e.g., the diffusion equation. For this reason, I would like to have a very short discussion on the PDEs. I refer the interested reader to chapter 19 of Numerical Recipes.

Partial differential equations are at the heart of many, if not most, computer analysis or simulations of continuous physical systems, such as ﬂuids, electromagnetic ﬁelds, etc. In most mathematics books, partial differential equations (PDEs) are classiﬁed into the three categories, hyperbolic, parabolic, and elliptic, on the basis of their characteristics, or curves of information propagation. The prototypical example of a hyperbolic equation is the one-dimensional wave equation

where v = constant is the velocity of wave propagation. The prototypical parabolic equation is the diffusion equation

where **D** is the diffusion coefﬁcient.

The prototypical elliptic equation is the Poisson equation

where the source term **ρ** is given. If the source term is equal to zero, the equation is Laplace’s equation. From a computational point of view, the classiﬁcation into these three canonical

From a computational point of view, the classiﬁcation into these three canonical types is not very meaningful. The first two equations both deﬁne initial value or Cauchy problems: If information on **u** (perhaps including time derivative information) is given at some initial time t0 for all **x**, then the equations describe how **u(x, t)** propagates itself forward in time. In other words, these two equations describe time evolution. The goal of a numerical code should be to track that time evolution with some desired accuracy. In** initial value problems**, one’s principal computational concern must be the *stability of the algorithm*. Many reasonable- looking algorithms for initial value problems just don’t work — they are numerically unstable.

By contrast, the third equation directs us to ﬁnd a single “static” function **u(x, y)** which satisﬁes the equation within some **(x, y)** region of interest, and which — one must also specify — has some desired behavior on the boundary of the region of interest. These problems are called **boundary value problems**. In contrast to initial value problems, stability is relatively easy to achieve for boundary value problems. Thus, *the efﬁciency of the algorithms*, both in computational load and storage requirements, becomes the principal concern.

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