|
|
Thread Tools | Display Modes |
#21
|
|||
|
|||
Velodrome banking helps how?
Tim McNamara wrote:
"Robert Chung" writes: That's a couple hundred watts difference between the straights and the turns. A couple *hundred* watts? Huh. Can you show us your math? Will showing you the data suffice? http://groups.google.com/group/rec.b...f12e35bb781e1c |
Ads |
#22
|
|||
|
|||
Velodrome banking helps how?
Phil Holman wrote:
"Robert Chung" wrote in message That's a couple hundred watts difference between the straights and the turns. Troll Do you know me, or what? --Robert, waiting for Het Volk. |
#23
|
|||
|
|||
Velodrome banking helps how?
Robert Chung wrote: Tim McNamara wrote: "Robert Chung" writes: That's a couple hundred watts difference between the straights and the turns. A couple *hundred* watts? Huh. Can you show us your math? Will showing you the data suffice? http://groups.google.com/group/rec.b...f12e35bb781e1c Could those figures come from distortions in the measurments due to the G's in the turn? Joseph |
#25
|
|||
|
|||
Velodrome banking helps how?
Robert Chung wrote: wrote: The only argument arises from purists who note that the rider does not travel the prescribed distance because they travel at a smaller radius than the surface of the track where the tires roll over the distance. That's a couple hundred watts difference between the straights and the turns. If this is true, do you suppose it is from increased RR, or does the rider have to climb their way through the turn in a way to overcome the acceleration, or does that not matter because the bike is just rolling along the contour of the track? Joseph |
#26
|
|||
|
|||
Velodrome banking helps how?
wrote:
Could those figures come from distortions in the measurments due to the G's in the turn? Hmmm. How would the G's affect a Power Tap? BTW, in the middle 1000m, power and speed were out-of-phase, i.e., speed increased as power was decreasing. Holman can tell you about floating the turns. McNamara will be able to show you the math. In the meantime: http://groups.google.com/group/rec.b...dd384c37b904e2 As a footnote to that latter post, in 2001 Tournant set the current world kilo record of 58.875 at La Paz. |
#27
|
|||
|
|||
Velodrome banking helps how?
Robert Chung wrote: wrote: Could those figures come from distortions in the measurments due to the G's in the turn? Hmmm. How would the G's affect a Power Tap? BTW, in the middle 1000m, power and speed were out-of-phase, i.e., speed increased as power was decreasing. Holman can tell you about floating the turns. McNamara will be able to show you the math. In the meantime: http://groups.google.com/group/rec.b...dd384c37b904e2 As a footnote to that latter post, in 2001 Tournant set the current world kilo record of 58.875 at La Paz. I don't know how a powertap works, so I don't know how it could be affected by G's. Unlikely I guess, as I imagine the folks at CycleOps know what they are doing. That is interesting about the acceleration out of the turns. I have only ridden on a velodrome a few times, so the whole experience was so strange I never got to think about how it really felt. A note on altitude: most of the current world speed skating records were set in Salt Lake City. Joseph |
#28
|
|||
|
|||
Velodrome banking helps how?
In article , Kinky Cowboy
) wrote: Why? On a velodrome, the tyre contact has to travel 1km, but the CG of the rider travels a bit less due to taking a tighter radius through the turns. This amounts to several metres per kilometre, and applies to the centre of pressure as well. Although the rolling resistance on the velodrome is higher, due to the increased normal load on the contact patches through the turns plus some camber drag/scrub as the bike is rarely exactly normal to the track surface, it is far from certain that a flat boarded straight track would be "at least as fast as a normal velodrome" The fastest times I've seen recorded for a fully-faired recumbent s/s 1 km have been on a flat runway rather than a velodrome - 58.13s by Sandro Bollina in a Lightning X2 at Interlaken in 1999. The winner of the unfaired class, however, clocked as near as make no odds the same time as he did the following year on a 250m wooden velodrome. At higher speeds it's difficult to hold one's steed low on the banking. -- Dave Larrington - http://www.legslarry.beerdrinkers.co.uk/ Like Kant, it is my wish to create my own individual epistemology. But I also wish to find out what is for pudding. |
#29
|
|||
|
|||
Velodrome banking helps how?
Dan Connelly wrote: Robert Chung wrote: Tim McNamara wrote: "Robert Chung" writes: That's a couple hundred watts difference between the straights and the turns. A couple *hundred* watts? Huh. Can you show us your math? Will showing you the data suffice? http://groups.google.com/group/rec.b...f12e35bb781e1c Okay, I'll try... hopefully I don't botch this one as much as my last attempt at posting calculations here (pedal force when climbing) . Given simplified assumptions (tires track each other, a planar path of the point of contact, system has time to approach dynamic equilibrium in corners, no effect of lean on bicycle aerodynamics) The lean angle in terms is a dynamic balance between the centrifugal force and the force of gravity (alternately, the bike is continuously falling into the turn). Centrifugal force: Mv^2/R Torque on bike: Mgz sin theta (theta == lean angle, z == initial height of COM) torque from centrifugal force: (Mv^2/R) z cos theta equate the two: Mv^2/R z cos theta = Mgz sin theta tan theta = v^2/(Rg) delta R (from lean) @ COM = z sin theta (1 - sin^2 theta) tan^2 theta = sin^2 theta = sin^2 theta (1 + tan^2 theta) = tan^2 theta = sin theta = tan theta / sqrt(1 + tan^2 theta) for 0 = theta pi/2 delta R (from lean) @ COM = z v^2/Rg / sqrt(1 + (v^2/Rg)^2) So, typical numbers: v = 13.9 mps g = 9.8 mps^2 R = 150 meters / 2 pi z = 1.2 meter delta R = 0.76 meters delta power / power = 1 - (1 - delta R / R) ** 3 = 9.3% So in this calculation, I get a 9.3% reduction in power due to wind resistance in the turn, assuming the tires follow the reference line, due to a 63 cm reduction in the path followed by the center of mass, assuming the center of aerodynamic resistance is at the center of mass. If the cyclist is outputting 400 watts, this represents a 3.7 watt savings while in the corner. Dan Nice. 3.7 saved from wind, but how much more RR? Joseph |
#30
|
|||
|
|||
Velodrome banking helps how?
Dan Connelly wrote:
Given [...] system has time to approach dynamic equilibrium in corners, http://anonymous.coward.free.fr/rbr/schwartzpursuit.png |
Thread Tools | |
Display Modes | |
|
|
Similar Threads | ||||
Thread | Thread Starter | Forum | Replies | Last Post |
San Diego Velodrome Swap Meet Sun April 10 | [email protected] | Racing | 4 | April 10th 05 05:07 AM |
Forest City Velodrome | Myfirstname Mylastname | Racing | 0 | April 1st 05 07:56 AM |
Riding a Coker in the dark on a velodrome during a freezing winters night | GizmoDuck | Unicycling | 11 | June 30th 04 07:51 AM |
Velodrome Unicycling | GizmoDuck | Unicycling | 22 | January 28th 04 01:16 AM |
Poor surface may close Northbrook's Velodrome | tracker140 | Racing | 4 | July 31st 03 08:55 PM |