The second equation gives . Differentiating it gives . Substitution into the first equation cancels the terms and the constant forcing, leaving . HenceThis has two independent constants, as expected for the first-order linear system of differential equations. At zero, the conditions give and . Thus the required particular solution isChecking directly, , while . This also verifies the signs introduced during elimination.
On an interval with , an integrating factor is . Multiplication givesIntegration therefore yieldsThe polynomial formula has a smooth continuation at , but the original coefficient is undefined there. Solution intervals for the stated equation must avoid that point, and the constants on its two sides need not agree.
The logarithm requires for real-valued solutions. Put . Since , the equation becomes . For a nonzero branch, separation givesRenaming the constant and restoring givesDividing by would omit the equilibrium , so the full solution set also includes . The nonzero branches are defined on connected intervals with and . A regular solution cannot switch from a nonzero branch to zero at an ordinary point, because the right-hand side is locally Lipschitz in there. These domain restrictions are part of the full real solution.
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