1.2 Integrals as General and Particular Solutions
The first-order equation takes an especially simple form if the right-hand-side function f does not actually involve the dependent variable y, so
In this special case we need only integrate both sides of Eq. (1) to obtain
This is a general solution of Eq. (1), meaning that it involves an arbitrary constant C, and for every choice of C it is a solution of the differential equation in (1). If G(x) is a particular antiderivative of f—that is, if
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