Solution

ID: past-exam-of-the-mathematics-course-of-the-year-1-of-the-natural-sciences-course-of-the-university-of-cambridge/2024/paper-1/13/b/ii/solution

Multiplying the ordinary differential equation by the nonzero integrating factor from part (i) makes its left-hand side . Hence the potential is constant:
Since for every real , this is equivalent to the explicit general solution
It is defined for all real . There are no lost solutions, since the integrating factor and the coefficient of are everywhere nonzero.

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