On a nonconstant branch with , regard as a function of . The equation becomes the linear ordinary differential equationAn integrating factor is , givingTaking an antiderivative yields the implicit familyOn a regular branch this can also be written . The latter form loses the constant solutions , which must be restored separately.
The implicit relation is a first integral of an ordinary differential equation: along any differentiable solution of the original equation,Conversely, a differentiable graph satisfying this relation solves the original equation wherever . The original equation is undefined when ; points at which also need separate attention before solving explicitly for . This is why dividing immediately by can lose valid solutions and obscure nonuniqueness.
The initial data force , so the implicit relation factors as . Near this permits either the constant branch or the sine branch:Both satisfy the original equation, including its degenerate value at the initial point. They have different slopes there, zero and one, so the initial value problem is not unique. There are no further differentiable local branches through that point: away from the two factors cannot switch, and joining the two different branches at zero would give unequal one-sided derivatives.
Again . Since the initial sine is nonzero, the local branch must satisfy . Selecting the inverse-sine branch through givesThis passes through the specified point and has , which verifies the original equation on this interval.
Here as well, but the branch through is the other inverse-sine branch:Its derivative is , and both the sign of and the original equation agree with this choice.
The characteristic equation of the associated homogeneous linear differential equation is . A constant particular integral is , soThe first boundary condition gives . The second gives . Eliminating yields , hence and . Therefore
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