Page 178 - Foundations Of Differential Calculus
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8. On the Higher Differentiation of Differential Formulas  161
             with no differential being constant, and the expression

                                        2     2    2
                                      dx + dy
                                     2 2
                                                 2
                                   dx d y − dx dy d x
             becomes equivalent to the proposed expression.
                                        3
                                            2
          V. Let the given expression be dx d y/d y, in which the differential dx is
             assumed to be constant. We let dy = pdx, dp = qdx, and dq = rdx.
                           2
                                                                     2
                   2
                                         3
                                 3
             Since d y = qdx and d y = rdx , the given formula becomes rdx /q.
             Now for q and r we substitute those values that they receive when no
             differential is assumed to be constant, that is,
                                         2
                                                 2
                                      dx d y − dy d x
                                  q =
                                           dx 3
             and
                                                  2 2
                           2 3
                                      2
                                                              3
                                         2
                         dx d y − 3dx d xd y +3dy d x − dx dy d x
                     r =                                        .
                                           dx 5
             We then obtain the following expression, which is equivalent to that
             originally given:
                          2 3        2  2        2 2        3
                        dx d y − 3dx d xd y +3dy d x − dx dy d x
                                        2
                                                2
                                    dx d y − dy d x
                                     3       3
                              dx dx d y − dy d x     2
                            =                    − 3d x.
                                    2
                                            2
                                dx d y − dy d x
        274. If we consider these transformations more carefully, we can find a
        more expeditious method in which it is not necessary to resort to the letters
        p, q, r, etc. Depending on which differential in the formula is assumed to
        be constant, different methods are used. First, suppose that the constant
        differential is dx. When we have substituted pdx for dy and conversely
        dy/dx for p, whenever the differentials dx or dy occur, they are retained
                                          2
        without alteration. However, wherever d y occurs, after we have substituted
            2
        qdx and then for q we have written the value
                          2
                                  2
                                                       2
                       dx d y − dy d x         2    dy d x
                                         or   d y −       ,
                             dx                       dx
                                                                       3
        the transformation is complete. Furthermore, if in the given expression d y
                                         3
        occurs, since we have substituted rdx , because of the value already found
                       3
        for r, whenever d y is found we write
                                                      3
                                             2 2
                                   2
                                2
                         3    3d xd y   3dy d x   dy d x
                        d y −         +         −       .
                                dx        dx 2      dx
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