  We incorporate the Seiberg-Witten map of noncommutative theory in the
classical London theory of type-I superconductivity when an external magnetic
field is applied. After defining the noncommutative Maxwell potentials, we
derive the London equation for the supercurrent as a function of the
noncommutative parameter, up to second order in gauge fields expansion. Keeping
track of the effects of noncommutative gauge fields, we argue that
noncommutative magnetic field effects can be cast in the permeability of the
superconductor as an emergent property of the material, measurable in possible
not-so-far ultra-high-energy experimental setups. Another consequence of the
Seiberg-Witten map is the London penetration length that acquires corrections
in the expansion. Also, we show that the flux quantization remains consistent
relative to the commutative case. Our effective magnetic permeability and
London penetration length reduce to the standard ones in the commutative limit.
