Use the complex potential of a two-dimensional potential flow convention , for which . A positive circulation is counterclockwise. The two point vortices and the two-dimensional point sink give
Branch choices change additive constants, not the local velocity field. A vortex is transported by the nonsingular velocity due to the other vortex and the sink; its own singular term is omitted. At this gives
The other vortex follows by symmetry. Put , with and . Multiplication by gives
For , integration yields
Equivalently, with ,
The curves obey , so they are logarithmic spirals. At , both vortices reach the sink at the origin. For nonzero circulation they make infinitely many turns in that finite time; for zero circulation they approach radially. The point-vortex evolution becomes singular at capture, so the formula does not define a regular continuation through the event.
Figure 1.
Two equal vortices spiral symmetrically into a central sink and reach it at a finite capture time
. Details.
Put and take the positive-frequency branch for . The phase velocity and group velocity are
Since the square root is increasing, minimizing is equivalent to minimizing . Its derivative is , which changes sign from negative to positive at
The phase speed diverges at both positive endpoints and , so this stationary point is its global minimum. At , , giving
The relative speed is especially transparent:
A narrow wave packet moves with , while its crests move with . For , : crests move forward through the packet, from its rear towards its front. For , : crests drift backwards relative to the packet, although both absolute velocities are positive. At the leading-order relative drift vanishes. This is the minimum phase speed of a gravity-capillary wave.
Figure 1.
Phase and group speeds cross at the minimum phase speed; crest drift relative to the packet reverses there
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