A series of laboratory experiments in a thermally driven, rotating fluid annulus are presented that investigate the onset and characteristics of phase synchronization and frequency entrainment between the intrinsic, chaotic, oscillatory amplitude modulation of travelling baroclinic waves and a periodic modulation of the (axisymmetric) thermal boundary conditions, subject to timedependent coupling. The time-dependence is in the form of a prescribed duty cycle in which the periodic forcing of the boundary conditions is applied for only a fraction d of each oscillation. For the rest of the oscillation, the boundary conditions are held fixed. Two profiles of forcing were investigated that capture different parts of the sinusoidal variation and d was varied over the range 0:1 d 1. Reducing d was found to act in a similar way to a reduction in a constant coupling coefficient in reducing the width of the interval in forcing frequency or period over which complete synchronization was observed (the "Arnol'd tongue") with respect to the detuning, although for the strongest pulse-like forcing profile some degree of synchronization was discernible even at d ¼ 0:1. Complete phase synchronization was obtained within the Arnol'd tongue itself, although the strength of the amplitude modulation of the baroclinic wave was not significantly affected. These experiments demonstrate a possible mechanism for intraseasonal and/or interannual "teleconnections" within the climate system of the Earth and other planets that does not rely on Rossby wave propagation across the planet along great circles. Synchronization is commonly discussed in the context of discrete, coupled oscillators which may be periodic or chaotic. But under some circumstances, extended nonlinear systems which are formally infinite-dimensional, such as fluid flows, may exhibit discrete oscillations and behave as if they consisted of discrete oscillating components. We study such an example in the laboratory, consisting of amplitude-modulated, azimuthally travelling baroclinic waves in a thermally driven, rotating annulus experiment. Earlier experiments showed that, under conditions in which the unperturbed travelling waves are spontaneously (either periodically or weakly chaotically) modulated in time, the amplitude modulation of the waves can be phase-locked and synchronized with periodic perturbations of the applied (axisymmetric) temperature difference between the inner and outer cylinders of the experiment. We use this potentially synchronized system to explore what happens if the periodic perturbations are applied for only a given fraction of each cycle-i.e., for a duty cycle <100%. Our systematic exploration of variations in both the duty cycle and detuning (difference in period between the natural oscillation period and that of the imposed boundary temperature variations) shows that the duty cycle acts in the same way as a variable coupling coefficient, demonstrating a narrowing of the frequency interval over which complete phase synchronization is observed as ...