Page 121 - Foundations Of Differential Calculus
P. 121

104    6. On the Differentiation of Transcendental Functions
        It follows that

                                                        2  2
                 dp   dq      −q          pdx      − p + q   dx
                    −    =   √       −   √       =     √        .
                 p    q    2p 1 − x 2  2q 1 − x 2   2pq 1 − x 2
              2    2
        Since p + q = 4 and pq =2x,wehave
                                          dx
                                 dy = − √       .
                                       x 1 − x 2
        This differential can more easily be found if the given logarithm is trans-
        formed by rationalization as follows:
                               √
                            1+   1 − x 2     1      1
                      y =ln            =ln     +      − 1 .
                                x            x     x 2
        If we let

                                    1      1
                                p =   +      − 1,
                                    x     x 2
        then
                                                              √

               −dx        dx       −dx       dx      −dx 1+     1 − x 2
          dp =      −   	       =      −   √       =       √          .
                x 2    3   1       x 2   x 2  1 − x 2    x 2  1 − x 2
                      x   x 2 − 1
        Since                           √
                                     1+   1 − x 2
                                 p =            ,
                                         x
        we have
                                    dp     −dx
                               dy =    = √        ,
                                    p    x 1 − x 2
        as we have already seen.

        184. Since the first differentials of logarithms, when divided by dx, are
        algebraic quantities, the second differentials and those of higher orders can
        easily be found with the rules of the previous chapter, provided that we
        assume that the differential dx is constant. Hence, if we let y =ln x, then
                               dx               dy   1
                          dy =         and        =   ,
                               x               dx    x
                                                2
                          2    −dx 2           d y   −1
                         d y =         and        =     ,
                                x 2            dx 2  x 2
                                  3             3
                          3    2dx             d y   2
                         d y =         and        =    ,
                                x 3            dx 3  x 3
                                                4
                          4    −6dx 4          d y   −6
                         d y =         and        =     ,
                                 x 4           dx 4  x 4
   116   117   118   119   120   121   122   123   124   125   126