Page 89 - Foundations Of Differential Calculus
P. 89

72    4. On the Nature of Differentials of Each Order
        differential calculus contains a method for finding all differentials of each
        order. From the word differential, which denotes an infinitely small differ-
        ence, we derive other names that have come into common usage. Thus we
        have the word differentiate, which means to find a differential. A quantity
        is said to be differentiated when its differential is found. Differentiation
        denotes the operation by which differentials are found. Hence differential
        calculus is also called the method of differentiating, since it contains a way
        of finding differentials.
        139. Just as in differential calculus the differential of any quantity is
        investigated, so there is a kind of calculus that consists in finding a quantity
        whose differential is one that is already given, and this is called integral
        calculus. If any differential is given, that quantity whose differential is the
        proposed quantity is called its integral. The reason for this name is as
        follows: Since a differential can be thought of as an infinitely small part by
        which a quantity increases, that quantity with respect to which this is a
        part can be thought of as a whole, that is, integral, and for this reason is
        called an integral. Thus, since dy is the differential of y, y, in turn, is the
                           2                                          2
        integral of dy. Since d y is the differential of dy, dy is the integral of d y.
                  2                  3       3                  4
        Likewise, d y is the integral of d y, and d y is the integral of d y, and so
        forth. It follows that any differentiation, from an inverse point of view, is
        also an example of integration.

        140. The origin and nature of both integrals and differentials can most
        clearly be explained from the theory of finite differences, which has been
        discussed in the first chapter. After it was shown how the difference of
        any quantity should be found, going in reverse, we also showed how, from
        a given difference, a quantity can be found whose difference is the one
        proposed. We called that quantity, with respect to its difference, the sum
        of the difference. Just as when we proceed to the infinitely small, differences
        become differentials, so the sums, which there were called just that, now
        receive the name of integral. For this reason integrals are sometimes called
        sums. The English call differentials by the name fluxions, and integrals are
        called by them fluents. Their mode of speaking about finding the fluent of
        a given fluxion is the same as ours when we speak of finding the integral
        of a given differential.
        141. Just as we use the symbol d for a differential, so we use the symbol

          to indicate an integral. Hence if this is placed before a differential, we
        are indicating that quantity whose differential is the one given. Thus, if the
        differential of y is pdx, that is, dy = pdx, then y is the integral of pdx.

        This is expressed as follows: y =  pdx, since y =  dy. Hence, the integral

        of pdx, symbolized by  pdx, is that quantity whose differential is pdx.
                          2
                                                                       2
        In a similar way if d y = qdx, where dp = qdx, then the integral of d y

        is dy, which is equal to pdx. Since p =  qdx,wehave dy = dx qdx,

        and hence y =  dx   qdx. If in addition, dq = rdx, then q =  rdx and
   84   85   86   87   88   89   90   91   92   93   94