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Differential and Integral Equation




                    Notes                          dx     dy
                                                 P 2   Q 2   R 2 = 0
                                                    dz    dz
                                             dx     dy
                                   Solving for    and
                                             dz     dz
                                                             dx    Q R   Q R   dy  R P  P R
                                                                 =   1  2  2  1  ,  1 2  1  2
                                                             dz     P Q  Q P   dz  P Q  Q P
                                                                     1  2  1 2      1  2  1 2
                                   hence
                                                         dx            dy         dz
                                                                 =                                         ...(2)
                                                     Q R   Q R      R P  P R  P Q   P Q
                                                       1  2  2  1    1 2  1  2  1  2  2  1
                                   i.e. equations (1) can be put in the form

                                                             dx     dy  dz
                                                                 =                                         ...(3)
                                                             P      Q   R
                                   Hence forth the equations (3) will be taken as the standard form of a pair of ordinary simultaneous
                                   equations of the first order and of the first degree.

                                                             dx     dy  dz
                                   Solution of                   =
                                                             P      Q    R
                                   We have
                                                             dx     dy  dz  ldx mdy ndz
                                                                 =                                         ...(4)
                                                             P      Q   R   lP mQ nR

                                   and if           lP mQ nR = 0                                           ...(5)

                                   then            ldx mdy ndz = 0                                         ...(6)
                                   and if (5) is an exact differential, say du, then u = a is one equation of the complete solution.

                                   Similarly choosing  ,l m  and  n  such that

                                                    l P m Q n R = 0.

                                   then           l dx m dy n dz = dv  0                                   ...(7)
                                   Whence v = b is another equation of the complete solution.
                                   This method may be used with advantage in some examples to obtain a zero denominator and
                                   a numerator that is an exact differential or a non-zero denominator of which the numerator is
                                   the differential.


                                          Example 1: Solve
                                                           dx        dy      dz
                                                                 =          2   2                          ...(1)
                                                          ( z x y )  ( z x y )  x  y

                                   Each fraction is equal to
                                                                         xdx y dy zdz        xdx y dy zdz
                                                                 =                    2   2
                                                                    xz (y x ) yz (x y ) z (x  y  )  0




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