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equation that relates the independent variable x, the dependent variable y and derivatives
                   of y is called an ordinary differential equation. Some examples of ODEs are:

                                                            0
                                                           y = y
                                                        00
                                                       y + y = cos x
                                                             2 0
                                                      3 00
                                                    x y + x y − 1 = 0
                                                                       000
                                                                    00
                                                                 0
                   In general, an ODE can be written as F(x, y, y , y , y , . . . ) = 0.
                       The key defining property of a partial differential equation (PDE) is that there is more
                   than one independent variable x, y, . . . There is a dependent variable that is an unknown
                   function of these variables u(x, y, . . .). We will often denote its derivatives by subscripts;
                   thus ∂u/∂x = u x , and so on. A PDE is an identity that relates the independent variables,
                   the dependent variable u, and the partial derivatives of u. It can be written as

                                 F(x, y, u(x, y), u x (x, y), u y (x, y)) = F(x, y, u, u x , u y ) = O.  (1.1)


                   This is the most general PDE in two independent variables of first order. The order of an
                   equation is the highest derivative that appears. The most general second-order PDE in
                   two independent variables is


                                             F(x, y, u, u x , u y , u xx , u xy , u yy ) = 0.        (1.2)

                   A solution of a PDE is a function u(x, y, . . .) that satisfies the equation identically, at least
                   in some region of the x, y, . . . variables. When solving an ordinary differential equation
                   (ODE), one sometimes reverses the roles of the independent and the dependent variables
                                                                 3
                   — for instance, for the separable ODE  du  = u . For PDEs, the distinction between the
                                                          dx
                   independent variables and the dependent variable (the unknown) is always maintained.
                   Some examples of PDEs (all of which occur in physical theory) are:

                      1) u x + u y = 0 (transport);

                      2) u x + yu y = 0 (transport);

                      3) u x + uu y = 0 (shock wave);

                      4) u xx + u yy = 0 (Laplace’s equation);

                                      3
                      5) u tt − u xx + u = 0 (wave with interaction);
                      6) u t + uu x + u xxx = 0 (dispersive wave);

                      7) u tt + u xxxx = 0 (vibrating bar);

                                            √
                      8) u t − iu xx = 0 (i =  −1) (quantum mechanics).
                   Each of these has two independent variables, written either as x and y or as x and t.
                   Examples 1 to 3 have order one; 4, 5, and 8 have order two; 6 has order three; and 7 has
                   order four. Examples 3, 5, and 6 are distinguished from the others in that they are not
                   ”linear.” We shall now explain this concept.



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