A theory is developed of the intricately fingered patterns of flux dom
ains observed in the intermediate state of thin type-I superconductors
. The patterns are shown to arise from the competition between the lon
g-range Biot-Savart interactions of the Meissner currents encircling e
ach region and the superconductor-normal surface energy. The energy of
a set of such domains is expressed as a nonlocal functional of the po
sitions of their boundaries, and a simple gradient flow in configurati
on space yields branched flux domains qualitatively like those seen in
experiment. Connections with pattern formation in amphiphilic monolay
ers and magnetic fluids are emphasized.