The separable differential equation gives . Thus on , and the initial value gives . Hence
The initial-value branch cannot cross its singularity at zero.
Multiplication by gives . Integrating and imposing yields . Therefore
On an interval avoiding zero put . A real solution requires , and the principal square root is . The homogeneous first-order differential equation reduces to
Where , separation of variables gives . Thus the nonconstant pieces are
restricted to intervals where the cosine of the phase is nonnegative. This sign condition is essential when substituting back into the original square root.
There are also the solutions and . They can join the nonconstant pieces with a continuous first derivative, because the transformed rate vanishes but is not Lipschitz continuous at . For example, on the positive axis every gives
The sticking solutions of a bounded square-root differential equation describe the same joining mechanism on either half-axis after using the increasing variable .
Near the initial point, division by gives . An integrating factor is , and
Thus , and gives
Although division by was local, direct substitution verifies this smooth solution in the original equation for every real , including the zeros of .
Set , so . The equation becomes . For its integrating factor is , giving
The initial value is , forcing . Hence
Substitution into the original equation verifies this answer throughout , including where the divided linear equation was singular. Its maximal connected interval through the initial point is .

Articles by others on the same topic (0)

There are currently no matching articles.