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100    6. On the Differentiation of Transcendental Functions
        180. We are investigating the differential of the hyperbolic logarithm of x
        and we let y =ln x, so that we have to define the value of dy. We substitute
                                              I
        x + dx for x so that y is transformed into y = y + dy. From this we have

                                                                dx
            y + dy =ln (x + dx) ,  dy =ln (x + dx) − ln x =ln 1+    .
                                                                 x
                              1
        But we have seen before that the hyperbolic logarithm of this kind of
        expression 1 + z can be expressed in an infinite series as follows:
                                        2    3   4
                                       z    z   z
                        ln (1 + z)= z −  +    −    + ··· .
                                       2    3    4
        When we substitute dx/x for z we obtain
                                 dx   dx 2  dx 3
                            dy =    −     +     − ··· .
                                 x    2x 2  3x 3
        Since all of the terms of this series vanish in the presence of the first term,
        we have
                                             dx
                                 d ln x = dy =  .
                                              x
        It follows that the differential of any logarithm whatsoever that has the
        ratio to the hyperbolic logarithm of n : 1, has the form n dx/x.
        181. Therefore, if ln p for any function p of x is given, by the same argu-
        ment, we see that its differential will be dp/p. Hence, in order to find the
        differential of any logarithm we have the following rule:
          For any quantity p whose logarithm is proposed, we take the differential
        of that quantity p and divide by the quantity p itself in order to obtain the
        desired differential of the logarithm.
          This same rule follows from the form
                                      0   0
                                     p − 1
                                            ,
                                        0
                                                              2
        to which we reduced the logarithm of p in the previous book. Let ω =0,
                        ω
        and since ln p =(p − 1)/ω,wehave
                                    1  ω   ω−1     dp
                           d ln p = d p = p   dp =   ,
                                   ω               p
        since ω = 0. It is to be noted, however, that dp/p is the differential of the
        hyperbolic logarithm of p, so that if the common logarithm of p is desired,
        this differential dp/p must be multiplied by the number 0.43429448 ... .

          1 Introduction, Book I, Chapter VII.
          2 Introduction, Book I, Chapter VII.
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