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#11
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"The Stability of the Bicycle"
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#12
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"The Stability of the Bicycle"
wrote in message ... Simon Brooke writes: There are a few simple tests that he didn't do, one of which is to wheel the bicycle along a walking speed holding on to the saddle only. Most bicyclists have done this and those who were interested will note that it works by gyroscopic force and not working at all with no wheel rotation. the effects of the steering geometry doesn't work with the bike stationary either. Uhhhmmmm... I habitually wheel bicycles with one hand on the saddle. I've always assumed that this worked in exactly the same way as riding a bike - i.e. lean to steer. Although I agree that in principle a rotating wheel has a gyroscopic effect at whatever speed it's rotating (and a fast spinning wheel a considerable one) I don't believe that there's much gyroscopic effect at this speed. Take the wheel out, spin it in you hands and try to tilt it to the left or right and note the force of the steering action. This should convince you of its effect. You don't need to solve differential equations. That's true, but does it prove thats what keeps the bike upright? Does it prove that the force you feel with a wheel is strong enough to keep a bike upright (esp with the extra forces of a rider). The "push a bike" experiment doesn't eliminate the effect of steering geometry. Does a bike with twice the rotating mass have the same stability at half the speed? |
#13
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"The Stability of the Bicycle"
There is more to be gained by
sending the researcher an electric motor and duh computer set up. call macarthur!!! we gotta get to the bottom of this. or its intersections! avast the skew! |
#15
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"The Stability of the Bicycle"
Phil Holman writes:
The greater mass of the wheel, handlebars etc. forward of the steering axis compared to the rear of the steering axis is the reason for the low speed steering when wheeling and leaning a bicycle. This is the case when the bicycle is stationary also. Gyro forces do not become dominant until much greater speeds. I can see you are hypothesizing. Take the wheel out,spin it in your hands, and try leaning it from side to side. If you don't believe the strong steering forces you experience, try steering the bicycle while holding it by the saddle when it isn't rolling. You'll notice it does not steer. No I'm not hypothesizing, if the lean is initiated quickly with a stationary bicycle the steering will go in the reverse direction and when the lean angle is reached the mass imbalance will make the wheel turn in the required direction. Initiating the lean very slowly will reduce the reverse steering affect. One technique of steering a wheeled bicycle at low speed is by rapid leaning with overtravel and then lean reversal (whiplash) to steer the wheel in the required direction. I notice you didn't respond to the initial proposal that gyroscopic forces, even at low speed, make wheeling the bicycle holding onto only the saddle, possible. This is done without any tricks or sudden motions using the rotating wheel as a steering control. Jobst Brandt |
#16
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"The Stability of the Bicycle"
wrote in message ... Phil Holman writes: The greater mass of the wheel, handlebars etc. forward of the steering axis compared to the rear of the steering axis is the reason for the low speed steering when wheeling and leaning a bicycle. This is the case when the bicycle is stationary also. Gyro forces do not become dominant until much greater speeds. I can see you are hypothesizing. Take the wheel out,spin it in your hands, and try leaning it from side to side. If you don't believe the strong steering forces you experience, try steering the bicycle while holding it by the saddle when it isn't rolling. You'll notice it does not steer. No I'm not hypothesizing, if the lean is initiated quickly with a stationary bicycle the steering will go in the reverse direction and when the lean angle is reached the mass imbalance will make the wheel turn in the required direction. Initiating the lean very slowly will reduce the reverse steering affect. One technique of steering a wheeled bicycle at low speed is by rapid leaning with overtravel and then lean reversal (whiplash) to steer the wheel in the required direction. I notice you didn't respond to the initial proposal that gyroscopic forces, even at low speed, make wheeling the bicycle holding onto only the saddle, possible. This is done without any tricks or sudden motions using the rotating wheel as a steering control. I don't know what you imply by this statement. Gyroscopic forces are in play as long as the wheel is rotating. At what speed the gyroscopic force overcomes the mass imbalance may be a more constructive line of investigation. Phil Holman Jobst Brandt |
#17
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"The Stability of the Bicycle"
Take the wheel out, spin it in you hands and try to tilt it to the
left or right and note the force of the steering action. This should convince you of its effect. please explain. gyro reaction is _90 degrees to the applied force_. i.e. my front wheel, spinning "forwards" tries to tilt top rightwards when turned to the left. you seem to be implying that gyro recation is responsible for banking the bike to the left when steered left. jb |
#18
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"The Stability of the Bicycle"
jim beam wrote:
Take the wheel out, spin it in you hands and try to tilt it to the left or right and note the force of the steering action. This should convince you of its effect. please explain. gyro reaction is _90 degrees to the applied force_. i.e. my front wheel, spinning "forwards" tries to tilt top rightwards when turned to the left. you seem to be implying that gyro recation is responsible for banking the bike to the left when steered left. No, when you wheel the bike along holding onto the seat you steer by banking the bike and the turn is a reaction to the bank. Banking the bike to the left will tend to initiate a turn to the left. But the gyroscopic force is quite small when the wheel is spun at only walking speed and the geometry of the bike also results in the wheel turning left in response to a left bank (even when the wheel isn't rotating). I'd have to try this with a counter-rotating second front wheel (like on URB I) before concluding which is the dominant effect. |
#19
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"The Stability of the Bicycle"
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#20
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"The Stability of the Bicycle"
Jim Beam writes:
Take the wheel out, spin it in you hands and try to tilt it to the left or right and note the force of the steering action. This should convince you of its effect. please explain. gyro reaction is _90 degrees to the applied force_. i.e. my front wheel, spinning "forwards" tries to tilt top rightwards when turned to the left. you seem to be implying that gyro recation is responsible for banking the bike to the left when steered left. Not at all. I suggest that the wheel spinning forward steers to the left when tilted to the left and to the right when tilted to the right. This is the means by which the bicycle steers when walking the bike while held by the saddle and also what enables it to be ridden no-hands. Jobst Brandt |
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