The noise voltage across a current-carrying type-I superconductor is attributed to flux flow. Measurements of power spectra of this flux-flow noise on In-2 at.% Pb foils show that the noise spectrum has a 1f^α frequency dependence with 0.5<α<1. This can be accounted for by a model in which the flux moves in a jerky manner because of interaction with immobile normal regions. This causes a distribution of voltage-pulse duration times. It is concluded from the power spectra that the dc voltage V is caused by a flux-flow component and an ohmic-loss voltage in immobile normal regions. The flux-flow fraction of the dc voltage is found to be a rapidly decreasing universal function of VVₙ, where Vₙ is the normal-state voltage. The size of the moving normal domains is calculated from the noise voltage and the dc voltage, and is shown to increase with field in a range from 10³φ₀ to about 10⁵φ₀. At low fields, flux presumably moves as bundles of small flux tubes, as in type-II superconductors. Close to Tc a structure is found in the power spectra which may be associated with the motion of vortex rings.
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G. J. van Gurp (1969) studied this question.
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