Page 170 - Foundations Of Differential Calculus
P. 170

8. On the Higher Differentiation of Differential Formulas  153
        method of dealing with them be explained. Soon, now, we will show the
        method by means of which second and higher differentials can always be
        eradicated.
        264. If an expression contains a single variable x and its higher differ-
                2
                         4
                    3
        entials d x, d x, d x, etc. occur in the expression, then it can have no
        fixed meaning unless some first differential is set constant. Thus, let t be
                                                                   3
                                                           2
        that variable whose differential dt is set constant. Then d t =0, d t =0,
         4
        d t = 0, etc. We let dx = pdt, and p will be a finite quantity whose differ-
        ential is not affected by the unsettled signification of second differentials;
        furthermore, dp/dt will be a finite quantity. Let dp = qdt, and in a similar
        way dq = rdt, dr = sdt, etc. Here q, r, s, etc. are finite quantities with
        fixed signification. Since dx = pdt,wehave
                                 2             2
                                d x = dp dt = qdt ,
                                 3       2      3
                                d x = dq dt = rdt ,
                                 4       3      4
                                d x = dr dt = sdt ,
                                   ....
                                        2   3    4
        If these values are substituted for d x, d x, d x, and so forth, the whole
        expression will contain only finite expressions and the first differential of
        dt, nor will there be any unsettled signification.

        265. If x were a function of t, then in this way the quantity x could be
        completely eliminated, so that only the quantity t and its differential dt
        would remain in the expression. However, if t were a function of x, then
        x would also be a function of t. Nevertheless, this quantity x with its first
        differential dx can be retained in the calculation, provided that after the
        substitutions previously made for t and dt, the values expressed by x and
                                                                       n
        dx are restored. In order that this might become clearer, we will let t = x ,
                                   n
        so that the first differential of x will be held constant. Since dt = nx n−1 dx,
                         n−1
        we have p =1/ nx      and
                             − (n − 1) dx          n−1
                        dp =            = qdt = nqx   dx,
                                nx n
        so that
                                      − (n − 1)
                                  q =
                                        2 2n−1
                                       n x
        and
                          (n − 1) (2n − 1) dx         n−1
                     dq =                  = rdt = nrx   dx.
                                 2 2n
                                n x
        From this it follows that
                                   (n − 1) (2n − 1)
                                r =
                                        3 3n−1
                                       n x
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