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Chapter 6 Partial Differential Equations

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4 CHAPTER 6. PARTIAL DIFFERENTIAL EQUATIONS<br />

Linear partial differential equation’s are often classified as being of elliptic, hyperbolic, or<br />

parabolic type. What follows is a brief and heuristic discussion of some of the features that<br />

characterize these classifications of partial differential equations. Most of what is presented<br />

in this introduction will be made precise in subsequent chapters.<br />

Elliptic <strong>Equations</strong><br />

An example of an elliptic partial differential equation is Laplace’s equation,<br />

div grad u =0<br />

If u = u(x 1 , ··· ,x n ) and (x 1 , ··· ,x n ) are rectangular Cartesian coordinates, and w(x) =<br />

(w 1 , ··· ,w n ),<br />

grad u = ∇u =(u x1 , ··· ,u xn )<br />

div ⃗w = ∂w + ···+ ∂w<br />

∂x 1 ∂x n<br />

and so<br />

div grad u = ∇·∇u = ∇ 2 u =∆u = u x1 x 1<br />

+ ···+ u xnx n<br />

=0.<br />

The Laplacian of u, ∆u, provides a comparison of values of u at a point with values at<br />

neighboring points. To illustrate this idea consider the simplest case that u = u(x) and<br />

assume u xx (x) > 0. Let ũ denote the tangent line approximation to u. For h>0 and<br />

sufficiently small,<br />

u(x + h) > ũ(x + h) =u(x)+u ′ (x)h<br />

u(x − h) > ũ(x − h) =u(x) − u ′ (x)h<br />

and so<br />

u(x + h)+u(x − h)<br />

>u(x).<br />

2<br />

Roughly stated, u(x) is smaller than its average value at nearby points if u xx (x) > 0. In<br />

higher dimensions, say n = 2, the analogous statement is that if ∆u(x, y) > 0, then the<br />

average value of u at neighboring points, say on a circle about (x, y), is greater than u(x, y).<br />

If ∆u(x, y) < 0, then u(x, y) is greater than the average value of u on a circle about (x, y).<br />

If ∆u(x, y) = 0 then u(x, y) is equal to its average value on a circle about (x, y). (We<br />

will subsequently prove a theorem that makes these ideas rigorous.) More generally, if<br />

∆u(x) =0,x∈ Ω ⊂ R n , then u is equal to its average value at neighboring points everywhere<br />

in Ω. In a certain sense, this says that if u satisfies Laplace’s equation then u represents a<br />

state of equilibrium.

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