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Unit 22: Solution of Laplace Differential Equation




          22.3 Summary                                                                          Notes

              Laplacian operator is expressed in Cartesian spherical polar co-ordinates and cylindrical
               co-ordinates.

              The solution of Laplace equation in these co-ordinate systems is solved.
              Laplace differential  equations finds  its applications  in potential  problems,  in  wave
               propagation and diffusion and heat conduction processes.

          22.4 Keywords


          Method of Separation of Variables helps in finding the solution of Laplace differential equation
          in all the three co-ordinate systems.
          Partial Differential Equation involve one dependent variable which is a function of more than
          one independent variable.

          22.5 Review Questions

          1.   Solve Laplace s equation in cylindrical co-ordinates and independent of Z.
          2.   Solve

                   2 u
                  r      0
                r    r

               subject to the boundary conditions
                         u ( ) 0 at r  a
                           r
                          u
               and       r ( ) u 0  at r  2a
                           y
                         x
          3.   Solve for  U ( , ) distribution
                2    2
                 U    U  0
                x 2  y 2
               subject to the conditions

                   y
                        l
                                 x
                         y
               U (0, ) U ( , ) 0, U ( ,0) x  2
                           U
               and               0
                           y
                             y b
          4.   Find the potential U(r,  ) inside the spherical surface of radius R when its spherical surface
               is kept at fixed distribution
               U ( , ) U 0  cos
                 R
          Answers: Self  Assessment


                      2(3cos 2  1) r  2
                 r
          1.   U ( , )        3
                            3r


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