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Supplementary Problems


               u = iu    xx  on (0, l) with Dirichlet conditions at the ends. Separate variables and
                 t
               find its representation as a series.


               Exercise 187. Solve the diffusion problem u = ku                  xx  in 0 < x < l, with the
                                                                       t
               mixed boundary conditions u(0, t) = u (l, t) = 0.
                                                            x
                                                                   2
                                                           1 2 2
               Solution: The eigenvalues are (n + ) π /l and the eigenfuncfions are sin[(n +
                                                           2
                1 )πx/l] for n = 0, 1, 2, . . .
                2
               Exercise 188. Consider diffusion inside an enclosed circular tube. Let its length
               (circum-ference) be 2l. Let x denote the arc length parameter where −l ≤ x ≤ l.

               Then the concentration of the diffusing substance satisfies u = ku              xx  for −l ≤ x ≤
                                                                                     t
               l, u(−l, t) = u(l, t) and u (−l, t) = u (l, t). These are called periodic boundary
                                                              x
                                               x
               conditions.
                                                                       2
                 (a) Show that the eigenvalues are λ = (πn/l) for n = 0, 1, 2, 3, . . .
                (b) Show that the concentration is


                                                  ∞
                                            a 0  X            |pinx             |pinx      2 2    2
                                 u(x, t)=      +      (a cos          + b sin         )e −n π kt/l  .
                                                                          n
                                                        n
                                             2                   l                l
                                                  n=1
               Exercise 189. Solve the equation u = 17u , 0 < x < π, t > 0, with the
                                                             t
                                                                       xx
               boundary conditions u(0, t) = u(π, t) = 0 t ≥ 0, and the initial conditions
                                                          (
                                                            0    0 ≤ x ≤ π/2,
                                              u(x, 0) =
                                                            2, π/2 < x ≤ π.


               Exercise 190.
                 (a) Using the method of separation of variables, find a (formal) solution of the

                     problem
                                 u − ku   xx  = 0 0 < x < L, t > 0,
                                  t
                      u (0, t) = u (L, t) = 0 t ≥ 0,
                        x
                                     x
                                u(x, 0) = f(x) 0 ≤ x ≤ L,
                     describing the heat evolution of an insulated one-dimensional rod (Neumann
                     problem).

                (b) Solve the heat equation u = 12u            xx  in 0 < x < π, t > 0 subject to the
                                                     t
                     following boundary and initial conditions:

                                             u (0, t) = u (π, t) = 0, t ≥ 0,
                                               x
                                                           x
                                                                 3
                                             u(x, 0) = 1 + sin x,          0 ≤ x ≤ π.
                 (c) Find lim  t→∞   u(x, t) for all 0 < x < π, and explain the physical interpretation

                     of your result.


               Exercise 191.



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