For Rayleigh-B\'enard convection of a fluid with Prandtl number σ0ex0ex=0ex0ex1.4, we report experimental and theoretical results on a pattern selection mechanism for cell-filling, giant, rotating spirals. We show that the pattern selection in a certain limit can be explained quantitatively by a phase-diffusion mechanism. This mechanism for pattern selection is very different from that for spirals in excitable media.
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Plapp et al. (1998) studied this question.
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