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Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

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PDES: GENERAL AND PARTICULAR SOLUTIONSEach is a valid solution (the freedom of choice of <strong>for</strong>m arises from the fact that uis specified at only one point (1, 1), <strong>and</strong> not along a continuum (say), as in boundarycondition (i)). All three are particular examples of the general solution, which may bewritten, <strong>for</strong> example, asu(x, y) =x 2 y +3+g(x 2 y),where g = g(x 2 y)=g(p) is an arbitrary function subject only to g(1) = 0. For thisexample, the <strong>for</strong>ms of g corresponding to the particular solutions listed above are g(p) =0,g(p) =3p − 3, g(p) =1− p. ◭As mentioned above, in order to find a solution of the <strong>for</strong>m u(x, y) =f(p) werequire that the original PDE contains no term in u, but only terms containingits partial derivatives. If a term in u is present, so that C(x, y) ≠ 0 in (20.9),then the procedure needs some modification, since we cannot simply divide outthe dependence on f(p) to obtain (20.10). In such cases we look instead <strong>for</strong>a solution of the <strong>for</strong>m u(x, y) =h(x, y)f(p). We illustrate this method in thefollowing example.◮Find the general solution ofx ∂u∂x +2∂u − 2u =0. (20.15)∂yWe seek a solution of the <strong>for</strong>m u(x, y) =h(x, y)f(p), with the consequence that∂u∂x = ∂h df(p) ∂pf(p)+h∂x dp ∂x ,∂u∂y = ∂h df(p) ∂pf(p)+h∂y dp ∂y .Substituting these expressions into the PDE (20.15) <strong>and</strong> rearranging, we obtain(x ∂h) (∂x +2∂h ∂y − 2h f(p)+ x ∂p )∂x +2∂p h df(p) =0.∂y dpThe first factor in parentheses is just the original PDE with u replaced by h. There<strong>for</strong>e, ifh is any solution of the PDE, however simple, this term will vanish, to leave(x ∂p )∂x +2∂p h df(p) =0,∂y dpfrom which, as in the previous case, we obtainx ∂p∂x +2∂p ∂y =0.From (20.11) <strong>and</strong> (20.12) we see that u(x, y) will be constant along lines of (x, y) thatsatisfydxx = dy 2 ,which integrates to give x = c exp(y/2). Identifying the constant of integration c with p wefind p = x exp(−y/2). Thus the general solution of (20.15) isu(x, y) =h(x, y)f(x exp(− 1 y)), 2where f(p) is any arbitrary function of p <strong>and</strong> h(x, y) is any solution of (20.15).684

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