Abstract
This work outlines the creation of a model of a velodrome datum line constructed from two straights, two circular-arc bends, and four transition curves. Different transition curve options are outlined and contrasted with a model with no transition curves. The influence of velodrome geometry on the wheel speed, wheel acceleration, roll angle, roll rate, and power demand of a theoretical cyclist is presented. The results display similar wheel speeds and roll angles for different transition curves, with larger differences when compared to the no-transition-curve option. Greater differences are observed in the acceleration and roll rate, for which calculations are only possible when using a transition curve. Comparisons of the model with theodolite measurements of two velodromes show a mean minimum root mean square error of 0.0398 m. This work can be used to increase the accuracy of existing track-cycling analytic models.
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Abbreviations
- ′:
-
(Prime) derivative with respect to lap distance
- \(\mathop {}\limits^{ \cdot }\) :
-
(Over-dot) derivative with respect to time
- \(Y\) :
-
Track half width (m)
- \(R\) :
-
Track mid-bend radius (m)
- \(\kappa\) :
-
Curvature (/m)
- \(\psi\) :
-
Curve tangential angle (rad)
- \(a\) :
-
Scaling factor
- \(\tau\) :
-
Curve parameter (m)
- \({K}\) :
-
Transition curve curvature profile (/m)
- \(({x}_{\text{T}},{y}_{\text{T}})\) :
-
Coordinates of the transition curve (m, m)
- \(({x}_{\text{B}},{y}_{\text{B}})\) :
-
Coordinates of the bend (m, m)
- \(({x}_{S},{y}_{S})\) :
-
Coordinates of the straight (m, m)
- \(({x}_{\text{Tc}},{y}_{\text{Tc}})\) :
-
Coordinates of the transition curve centre of curvature (m, m)
- \(({x}_{\text{Bc}},{y}_{\text{Bc}})\) :
-
Coordinates of the bend centre of curvature (m, m)
- \({L}_{L}\) :
-
Length of the lap (m)
- \({L}_{\text{T}}\) :
-
Length of the transition curve (m)
- \({L}_{\text{B}}\) :
-
Length of the bend (m)
- \({L}_{\text{S}}\) :
-
Length of the straight (m)
- \(\beta\) :
-
Track bank angle (rad)
- \({V}_{\text{W}}\) :
-
Velocity of the wheels (m/s)
- \({V}_{\text{CG}}\) :
-
Velocity of the centre of gravity (m/s)
- \({V}_{\text{A}}\) :
-
Velocity of the air relative to the cyclist (m/s)
- \({a}_{\text{W}}\) :
-
Acceleration of the wheels (m/s2)
- \({a}_{\text{CG}}\) :
-
Acceleration of the centre of gravity (m/s2)
- \(\phi\) :
-
Roll angle (rad)
- \({C}_{\text{D}}A\) :
-
Aerodynamic drag area (m2)
- \({C}_{\text{RR}}\) :
-
Coefficient of rolling resistance
- \({\mu }_{\text{s}}\) :
-
Coefficient of scrubbing resistance (/rad)
- \(\eta\) :
-
Drivetrain efficiency
- \(\rho\) :
-
Air density (kg/m3)
- \({h}_{\text{CG}}\) :
-
Height of the centre of gravity (m)
- \(m\) :
-
Combined cyclist/bicycle mass (kg)
- \(g\) :
-
Gravitational acceleration (m/s2)
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Fitzgerald, S., Kelso, R., Grimshaw, P. et al. Impact of transition design on the accuracy of velodrome models. Sports Eng 24, 23 (2021). https://doi.org/10.1007/s12283-021-00360-3
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DOI: https://doi.org/10.1007/s12283-021-00360-3