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book   Mobk070    March 22, 2007  11:7








                                                          SOLUTIONS WITH LAPLACE TRANSFORMS         125
                   Problems
                      1. Solve the above vibration problem when

                                                         y(0,τ) = 0
                                                         y(1,τ) = g(τ)

                          Hint: To make use of convolution see Example 8.3.
                      2. Solve the problem

                                                     2
                                                            2
                                                    ∂ y    ∂ y
                                                        =
                                                    ∂t 2   ∂x 2
                                                 y x (0, t) = y(x, 0) = y t (x, 0) = 0
                                                  y(1, t) = h

                          using the Laplace transform method.

                   8.2    DIFFUSION OR CONDUCTION PROBLEMS
                   We now consider the conduction problem

                   Example 8.3.

                                                         u τ = u ςς
                                                      u(1,τ) = f (τ)
                                                      u(0,τ) = 0
                                                      u(ς, 0) = 0

                        Taking the Laplace transform of the equation and boundary conditions and noting that
                   u(ς, 0) = 0,

                                                      sU(s ) = U ςς
                   solution yields
                                                           √            √
                                                U = A sinh   s ς + B cosh  s ς
                                            U(0, s ) = 0

                                            U(1, s ) = F(s )

                        The first condition implies that B = 0 and the second gives
                                                                 √
                                                    F(s ) = A sinh  s
                                     √
                                      s ς
                   and so U = F(s ) sinh  √ .
                                   sinh  s
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