The complex velocity obtained from part (b) is
For a nonzero planar potential doublet, . Its zeros therefore satisfy
and hence
The denominators are nonzero because . For either sign,
so . They are distinct because and is injective, its determinant being . Clearing the velocity denominators gives a quadratic with these two roots, so there are no further finite stagnation points. Thus both stagnation points lie on the obstacle boundary.

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