The purpose of this article was to establish whether previously reported oxygen-to-mass ratios, used to predict flat and hill-climbing cycling performance, extend to similar power-to-mass ratios incorporating other, often quick and convenient measures of power output recorded in the laboratory [maximum aerobic power (W MAP ), power output at ventilatory threshold (W VT ) and average power output (W AVG ) maintained during a 1 h performance test]. A proportional allometric model was used to predict the optimal power-to-mass ratios associated with cycling speeds during flat and hill-climbing cycling. The optimal models predicting flat time-trial cycling speeds were found to be ( . Based on these models, there is evidence to support that previously reported _ V O 2 -tomass ratios associated with flat cycling speed extend to other laboratory-recorded measures of power output (i.e. Wm
À0.32). However, the power-function exponents (0.54, 0.46 and 0.58) would appear to conflict with the assumption that the cyclists' speeds should be proportional to the cube root (0.33) of power demand/ expended, a finding that could be explained by other confounding variables such as bicycle geometry, tractional resistance and/or the presence of a tailwind. The models predicting 6 and 12% hill-climbing cycling speeds were found to be proportional to (W MAP m À0.91 ) 0.66 , revealing a mass exponent, 0.91, that also supports previous research.Keywords Power supply and demand AE Cycling speed AE Maximal aerobic power (W MAP ) AE Power at ventilatory threshold (W VT ) AE Average power output (W AVG )