The magnetoconductance G in chaotic quantum dots at medium/high magnetic fl
uxes Phi is calculated by means of a tight-binding Hamiltonian on a square
lattice. Chaotic dots are simulated by introducing diagonal disorder on sur
face sites of L x L clusters. It is shown that when the ratio W/L is suffic
iently large, W being the width of the leads, G increases steadily (almost
with no fluctuations) showing a maximum at a magnetic flux Phi (max) propor
tional to L-2/W (a flux at which the cyclotron radius r(c) approximate to W
/2). Neither regular nor bulk disordered ballistic cavities (with a content
of impurities proportional to L) show this effect. On the other hand, for
magnetic fluxes such that r(c) > L/2 and up to the aforementioned maximum,
the average magnetoconductance increases almost linearly with the flux with
a slope proportional to W-2. These results closely follow a theory propose
d by Beenakker and van Houten to explain the magnetoconductance of two poin
t contacts in series.