Abstract
When a counterflow supercurrent is generated in a superconducting bimetallic loop by a thermoelectric quasiparticle current, the phase difference can only be maintained constant if very large surface currents flow. We show that this implies a magnetic flux associated with the loop of order $\frac{r}{\ensuremath{\lambda}}$ ($r$ is the radius of arm perpendicular to $\ensuremath{\nabla}T$ and $\ensuremath{\lambda}$ is the penetration depth) greater than the simple theory suggests, and that this may be used to m\'easure the normal current directly.
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