We consider the cosmology of a "3-brane universe" in a five dimensional (bu
lk) space-time with a cosmological constant. We show that Einstein's equati
ons admit a first integral, analogous to the first Friedmann equation, whic
h governs the evolution of the metric in the brane, whatever the time evolu
tion of the metric along the fifth dimension. We thus obtain the cosmologic
al evolution in the brane for any equation of state describing the matter i
n the brane, without needing the dependence of the metric on the fifth dime
nsion. In the particular case p = wp (w = constant), we give explicit expre
ssions for the time evolution of the brane scale factor, which show that st
andard cosmological evolution can be obtained (after an early non conventio
nal phase) in a scenario a la Randall and Sundrum, where a brane tension co
mpensates the bulk cosmological constant. We also show that a tiny deviatio
n from exact compensation leads to an effective cosmological constant at la
te time. Moreover, when the metric along the fifth dimension is static, we
are able to extend the solution found on the brane to the whole spacetime.
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