The homogeneous first-order differential equation suggests , so . Wherever the original equation is defined,
Thus the implicit solution is . The printed initial values force .
There is no classical solution through the printed initial point. There , so the tangent on the right is undefined. The implicit relation nevertheless has two neighboring real branches on which approach that point continuously:
Both tend to as , but their derivatives become unbounded with opposite signs. They solve the equation on the open interval , not at its endpoint. Other inverse-sine periods cannot approach the specified initial value. This is an endpoint obstruction in a homogeneous differential equation. Constant-ratio branches also solve the general equation where , but do not meet the initial data.

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