  We analyze the magnetic field of electroweak dumbbells. While the magnetic
field of the untwisted dumbbell is given by the usual dipole formula and falls
of as $1/r^3$, dumbbells with twist have a novel twisted magnetic field that
only falls off as $\cos\theta/r^2$ (in spherical coordinates). We comment on
the relevance of twisted electroweak dumbbells for understanding the coherence
of the magnetic field generated at the electroweak phase transition.
