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Sachin Kaushal, Lovely Professional University              Unit 22: Solution of Laplace Differential Equation





               Unit 22: Solution of Laplace Differential Equation                               Notes


            CONTENTS
            Objectives
            Introduction
            22.1 Solution of Laplace Differential Equation   Cylindrical Co-ordinates

            22.2 Circular Harmonics
                 22.2.1  Solution of Laplace s Equation in Spherical Polar Co-ordinates
                 22.2.2  Steady Flow of Heat in Rectangular Plate
            22.3 Summary
            22.4 Keywords
            22.5 Review Questions

            22.6 Further Readings
          Objectives


          After studying this unit, you should be able to:
              Know that Laplace equation is a partial differential equation involving one dependent
               variable and three independent variables.
              See that it has a vast number of applications in gravitational potential process in electrostatic
               potential  distributions,  in  the  propagation  of  waves,  in  diffusion  process  or  heat
               conductions.
              Note that three major co-ordinate systems namely the Cartesian co-ordinate system the
               spherical polar co-ordinate  system or the cylindrical  co-ordinate systems are used  to
               express Laplacian operator.

          Introduction

          This Laplace equation is seen to be written in such a way that the dependence of dependent
          variable on three independent variables can be separated.
          Both spherical polar co-ordinates and cylindrical co-ordinates are used to find the solution of
          Laplace equation.

          22.1 Solution of Laplace Differential Equation   Cylindrical

               Co-ordinates

          The  most important  partial differential equation of applied mathematics  is the  differential
          equation of Laplace i.e.
                          2
                          V  = 0                                                   ...(1)
                                                                      ,
                                                                    ,
          The Laplace operator is expressed in general curvilinear co-ordinates  u u u  in the following
                                                                   1
                                                                        3
                                                                     2
          manner,
                                  1        h h          h h          h h
                           2 =              2 3          3 1          1 2          ...(2)
                                h h h  u 1  h 1  u 1  u 2  h 2  u 2  u 3  h 3  u 3
                                 1 2 3
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