Prediction of passive and active drag in swimming

In order to understand the physical origin of passive resistance in swimming the resistance breakdown for a swimmer is investigated. A combination of empirical methods and theoretical analysis is used to predict passive resistance in the speed range 0 - 2 ms-1 and is shown to provide similar results...

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Bibliographic Details
Main Authors: Webb, A. (Author), Banks, Joseph (Author), Phillips, C.W.G (Author), Hudson, D.A (Author), Taunton, D.J (Author), Turnock, S.R (Author)
Format: Article
Language:English
Published: 2011-09.
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Online Access:Get fulltext
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042 |a dc 
100 1 0 |a Webb, A.  |e author 
700 1 0 |a Banks, Joseph  |e author 
700 1 0 |a Phillips, C.W.G.  |e author 
700 1 0 |a Hudson, D.A.  |e author 
700 1 0 |a Taunton, D.J.  |e author 
700 1 0 |a Turnock, S.R.  |e author 
245 0 0 |a Prediction of passive and active drag in swimming 
260 |c 2011-09. 
856 |z Get fulltext  |u https://eprints.soton.ac.uk/198795/1/Angus_Webb_APCST_2011.pdf 
520 |a In order to understand the physical origin of passive resistance in swimming the resistance breakdown for a swimmer is investigated. A combination of empirical methods and theoretical analysis is used to predict passive resistance in the speed range 0 - 2 ms-1 and is shown to provide similar results to those from experimental testing. Typical magnitudes of wave, viscous pressure and skin friction resistance contribute 59%, 33% and 8% of total passive resistance respectively at free swim speed. A comparison is made between the widely used Velocity Perturbation Method and a Naval Architecture based approach in predicting active drag. For the swimmer investigated the two approaches predict active drag of 131.4 N and 133.9 N for a swimming speed of 1.53 ms-1. However, the results predicted from the Velocity Perturbation Method have a much higher uncertainty and the Naval Architecture based approach is suggested as a more robust method of predicting active drag. 
655 7 |a Article