Page 185 - Foundations Of Differential Calculus
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168    9. On Differential Equations
        Since P and Q are functions of x, their differentials have the form dP = pdx
        and dQ = qdx so that
                          2ydy + Pdy + yp dx + qdx =0,

        with the result that
                                  dy     yp + q
                                     = −       .
                                  dx     2y + P

                                          2
        283. Now, just as the finite equation y +Py+Q = 0 gives the relationship
        between y and x, so the differential equation expresses the relationship, or
        the ratio of dy to dx. However since
                                  dy   −yp + q
                                     =         ,
                                  dx    2y + P
        we cannot know this ratio dy : dx unless we know the function y. Things
        could not possibly be otherwise, since from the finite equation y has two
        values. Either of these two values has its own proper differential, and either
        differential will appear depending on which value is substituted for y.Ina
        similar way, the function y can be defined by a cubic equation. In this case,
        dy/dx will have three values, depending on which of the three values of y
        is substituted. If in a given finite equation y has four or more values, then
        of necessity, dy/dx has just as many significations.
        284. Nevertheless, the function y can be eliminated, since we have two
        equations containing y, namely the finite and the differential. In that case,
        however, the differential dy will take on as many values as y had in the
        original finite equation. Thus there are this many ratios of dy to dx. Let
                                      2
        us take the preceding example, y + Py + Q = 0, whose differential is
        2ydy + Pdy + ydP + dQ = 0, from which we obtain
                                      Pdy + dQ
                                 y = −          .
                                       2dy + dP
        When this value for y is substituted in the previous equation, we have
                   2     2        2             2               2
             4Q − P  dy + 4Q − P    dP dy + QdP − PdPdQ + dQ =0,
        whose roots are
                                         1
                                   1     2 PdP − dQ
                                             2
                            dy = − dP ±             .
                                   2        P − 4Q
        These two differentials correspond to the two values of y from the original
        finite equation
                                   1    1
                                             2
                             y = − P +      P − 4Q.
                                   2    2
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