Scaling maximal oxygen uptake to predict cycling time-trial performance in the field: a non-linear approach.
dc.contributor.author | Nevill, Alan M. | |
dc.contributor.author | Jobson, Simon A. | |
dc.contributor.author | Palmer, G.S. | |
dc.contributor.author | Olds, Tim | |
dc.date.accessioned | 2007-01-25T16:03:07Z | |
dc.date.available | 2007-01-25T16:03:07Z | |
dc.date.issued | 2005 | |
dc.identifier.citation | European Journal of Applied Physiology, 94(5-6): 705-710 | |
dc.identifier.issn | 1439-6319 | |
dc.identifier.pmid | 15906080 | |
dc.identifier.doi | 10.1007/s00421-005-1321-8 | |
dc.identifier.uri | http://hdl.handle.net/2436/7755 | |
dc.description.abstract | The purpose of the present article is to identify the most appropriate method of scaling VO2max for differences in body mass when assessing the energy cost of time-trial cycling. The data from three time-trial cycling studies were analysed (N = 79) using a proportional power-function ANCOVA model. The maximum oxygen uptake-to-mass ratio found to predict cycling speed was VO2max(m)(-0.32) precisely the same as that derived by Swain for sub-maximal cycling speeds (10, 15 and 20 mph). The analysis was also able to confirm a proportional curvilinear association between cycling speed and energy cost, given by (VO2max(m)(-0.32))0.41. The model predicts, for example, that for a male cyclist (72 kg) to increase his average speed from 30 km h(-1) to 35 km h(-1), he would require an increase in VO2max from 2.36 l min(-1) to 3.44 l min(-1), an increase of 1.08 l min(-1). In contrast, for the cyclist to increase his mean speed from 40 km h(-1) to 45 km h(-1), he would require a greater increase in VO2max from 4.77 l min(-1) to 6.36 l min(-1), i.e. an increase of 1.59 l min(-1). The model is also able to accommodate other determinants of time-trial cycling, e.g. the benefit of cycling with a side wind (5% faster) compared with facing a predominately head/tail wind (P<0.05). Future research could explore whether the same scaling approach could be applied to, for example, alternative measures of recording power output to improve the prediction of time-trial cycling performance. | |
dc.format.extent | 282770 bytes | |
dc.format.mimetype | application/pdf | |
dc.language.iso | en | |
dc.publisher | Springer Berlin / Heidelberg | |
dc.relation.url | http://www.springerlink.com/content/j863561v70228548/ | |
dc.subject | Performance measurement | |
dc.subject | Sports Medicine | |
dc.subject | Power output | |
dc.subject | Allometric modelling | |
dc.subject | Cycling | |
dc.subject | Body mass | |
dc.subject | Wind resistance | |
dc.title | Scaling maximal oxygen uptake to predict cycling time-trial performance in the field: a non-linear approach. | |
dc.type | Journal article | |
dc.format.dig | YES | |
refterms.dateFOA | 2018-08-21T15:54:43Z | |
html.description.abstract | The purpose of the present article is to identify the most appropriate method of scaling VO2max for differences in body mass when assessing the energy cost of time-trial cycling. The data from three time-trial cycling studies were analysed (N = 79) using a proportional power-function ANCOVA model. The maximum oxygen uptake-to-mass ratio found to predict cycling speed was VO2max(m)(-0.32) precisely the same as that derived by Swain for sub-maximal cycling speeds (10, 15 and 20 mph). The analysis was also able to confirm a proportional curvilinear association between cycling speed and energy cost, given by (VO2max(m)(-0.32))0.41. The model predicts, for example, that for a male cyclist (72 kg) to increase his average speed from 30 km h(-1) to 35 km h(-1), he would require an increase in VO2max from 2.36 l min(-1) to 3.44 l min(-1), an increase of 1.08 l min(-1). In contrast, for the cyclist to increase his mean speed from 40 km h(-1) to 45 km h(-1), he would require a greater increase in VO2max from 4.77 l min(-1) to 6.36 l min(-1), i.e. an increase of 1.59 l min(-1). The model is also able to accommodate other determinants of time-trial cycling, e.g. the benefit of cycling with a side wind (5% faster) compared with facing a predominately head/tail wind (P<0.05). Future research could explore whether the same scaling approach could be applied to, for example, alternative measures of recording power output to improve the prediction of time-trial cycling performance. |