Macroscopic magnetic dipoles are considered as cosmic dark matter. Permanent
magnetism in relativistic field structures can involve some form of
superconductivity, one example being current-carrying string loops (springs') with vanishing net tension. We derive the cross section for free classical dipoles to collide, finding it depends weakly on orientation when mutual precession is rapid. The collision rate of spring’ loops with tension ${\cal
T} \sim 10^{-8}c^4/G$ in galactic halos approaches the measured rate of fast
radio bursts (FRBs) if the loops comprise most of the dark matter. A large
superconducting dipole (LSD) with mass g and size mm
will form a km magnetosphere moving through interstellar plasma.
Although hydromagnetic drag is generally weak, it is strong enough to capture
some LSDs into long-lived rings orbiting supermassive black holes (SMBHs) that
form by the direct collapse of massive gas clouds. Repeated collisions near
young SMBHs could dominate the global collision rate, thereby broadening the
dipole mass spectrum. Colliding LSDs produce tiny, hot electromagnetic
explosions. The accompanying paper shows that these explosions couple
effectively to propagating low-frequency electromagnetic modes, with output
peaking at 0.01-1 THz. We describe several constraints on, and predictions of,
LSDs as cosmic dark matter. The shock formed by an infalling LSD triggers
self-sustained thermonuclear burning in a C/O (ONeMg) white dwarf (WD) of mass
(). The spark is generally located well off
the center of the WD. The rate of LSD-induced explosions matches the observed
rate of Type Ia supernovae.

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