The gravitomagnetic clock effect is the difference in periods of a test par
ticle revolving in prograde and retrograde circular geodesic orbits around
a rotating body. We study this effect far a cylindrically symmetric system,
but our analysis also applies to orbits around the Kerr source in its plan
e of symmetry. The effect depends on the coordinate system, and we find the
condition that it can be reduced to zero by a suitable choice of rotating
axes.
We apply our formulae to the van Stockum metric for a rotating dust cylinde
r, and to the Kerr solution. In the former there is a gravitomagnetic clock
effect only in the case of low mass per unit length, and the coordinate sy
stem in which the effect vanishes is the one in which the distant stars wou
ld be at rest. In Kerr spacetime the gravitomagnetic clock effect can be ma
de to vanish, but only by choosing a frame rotating with respect to the dis
tant stars.