On an interval with , division by gives the separable differential equation . For , take antiderivatives:
Renaming the constant yields the explicit nonzero family
For , the interval of definition must avoid zeros of the denominator. Division by excluded the additional solution , which must also be included.
The original undivided differential equation also makes sense at , where it requires . For continuation through a zero of the leading ODE coefficient, rewrite the nonzero family as
It extends differentiably with and , since . One may choose the integration constants independently on the two sides of zero and obtain a differentiable solution through zero. The zero solution also extends through zero, with derivative ; joining a nonzero branch on just one side to a zero branch on the other would fail differentiability.
For this first-order linear differential equation, an integrating factor on an interval avoiding zeros of is . The product rule then gives
The initial condition gives , hence . Thus
The displayed interval is the maximal one containing the specified initial point, since the coefficient is undefined at its endpoints.
Use the substitution for a homogeneous first-order differential equation. Since , it gives
Where , this separable differential equation integrates to , hence . One can obtain the same relation without division by : the equation gives , so , including .
All real branches of the inverse sine are captured by
Each branch is used on an interval with and , with fixed . The strict inequality excludes zeros of , where the original tangent is undefined. When , the formula includes all straight-line solutions . Keeping both families of inverse sine branches is essential for the two different initial conditions below.
The initial condition gives . Since belongs to the principal inverse sine range, choose in part (i). The particular solution is
The upper endpoint is excluded because there and the original tangent ceases to be defined.
Again , but the principal inverse sine would give at . The required branch is , corresponding to . Therefore
At the bracket is , as required. Both the initial condition and the original differential equation are thus satisfied on the stated branch.

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