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why do we lose balance in a bike when at a standstill? |
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| Nov5-04, 02:03 PM | #35 |
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why do we lose balance in a bike when at a standstill? |
| Nov5-04, 03:51 PM | #36 |
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| Nov7-04, 11:29 AM | #37 |
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Can someone explain what exactly the gyroscopic action is?
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| Nov8-04, 04:16 AM | #38 |
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Using a helicopter as example, there's a cyclic control that changed the pitch of the blades as they travel around in a circle. If the cyclic is tilted forwards, creating a pitch down torque force, the helicopter instead responds with a roll towards the rearward rotating blades. If the cyclic is tilted sideways towards the forward rotating blades, the helicopter pitches down. To keep the pilot from getting confused, the cyclic control is shifted 90 degrees to compensate for this, so the pilot can just push forwards to pitch downwards. |
| Nov8-04, 09:58 AM | #39 |
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If you have ever ridden a bike on rollers, you will find out how very little help "conservation of angular momentum" will be for balance.
As opposed to stationary trainers, rollers are thin barrels that the wheels sit on. The rear wheel spins normally, which turns the rear roller, which is attached to a long band which turns the front roller which turns the front wheel. There is just as much angular momentum as when on the road. The wheels are not kept in place "side-to side" and consequently, a novice bicyclist will fall repeatedly, no matter how fast the wheels are spinning. The reason why rollers are more difficult than actually riding, is you just can't lean! Leaning will turn the front wheel which will send you 10 inches to the side and off you go! So angular momentum does connect the lean with the turn of the front wheel, but it does nearly nothing to keep us "gyroscopically" upright. (Basically, everything Krab has said is Bang on.) |
| Feb22-06, 03:09 PM | #40 |
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| Feb22-06, 07:21 PM | #41 |
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I don't know if I mentioned this before, but I can balance a 10 speed for about 10 to 30 seconds without moving. This is because steering the front tire translates the contact patch sideways. Steer left, and the contact patch move right if not resisted. With the front tire on the ground, the contact patch doesn't slide much, so steering left moves the front end left. It's enough movement to balance a bike, but it's difficult. Velodrome racers can remain still for very long times, as this is part of the tactic used to try and get the other racer(s) ahead for those racers that want to start from behind (draft). |
| Apr24-11, 03:42 PM | #42 |
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Let me throw in a controversial twist to this discussion. Someone pointed out that gyroscopic effects plays no part in bicycle's balancing and threw in the counter rotating added wheels argument to back it up. Someone disagreed with him and said if anything the gyroscopic stability will increase. The first guy insisted that angular momentum is a vector hence this cancels out blah blah blah (they lost me somewhere. I agree with whoever say gyroscopic stability will improve, intuitively though cause my phyisic background is wanting. Now to the twist and this is helped by a chap who said motion in itself yield stability and called to meind ice skaters among other wheel-less locomotion.
Mine is simple. Riding a bike a structured perpetual falling to a particular direction much like a satellite in orbit. Take a flag pole and stand it on a flat surface. It is highly unstable (an inveted pendulam-like) Now tip it to fall to one direction. It is extremly had now to make it fall to any other direction. Left to its own divices it will hit at an exact spot. Slowing a bicycle to a stop is analogous to standing the flag pole on its foot again. how about that for food for thought? |
| Apr24-11, 04:22 PM | #43 |
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I can't find any comments in this thread, about the effect of castor action and the fact that a line through the top bracket (the steering axis) on all stable bikes, when produced, always meets the ground ahead of the tyre footprint. This will always cause the wheel to steer into a lean. The result, when traveling forward, will be to produce a force on the ground, 'inwards' and a corresponding moment to turn the bike upright. The faster the bike is travelling, the more this effect will be.
Whilst the gyroscopic effect may be significant on morotbikes, it will be very small on light wheeled bikes - particularly with small diameter wheels, whereas the castor effect only depends on the distance between footprint and the forward produced line of the steering axis on the ground. Folding and 'delivery' bikes have very small front wheels but are still stable. It even works on kids' scooters with plastic wheels of less than 10cm diameter where angular momentum is extremely small. There is more to this than just one mechanism at work, I'm sure. |
| Apr24-11, 06:04 PM | #44 |
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| Sep22-11, 06:44 AM | #45 |
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| Sep22-11, 07:01 AM | #46 |
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That link is good and very inventive in its thesis. (I wonder how many takes they did to get that bike to stay up so well) At least it puts to bed the gyro theory, which applies to very few cases and which, I think only applies a damping / reactive force rather than a restoring force. If the gyro action were actually to bring the bike upright, would not the force be downwards again - by the same precession argument- as the rotation would then be the other way? Once a bike has leant into the curve, after the (truly) restoring couple is there until it is actually upright again.
"Turning into a fall" is a very good way of putting things; both "trail" and castor action, will achieve this. Their model has this forward pointing rod, which achieves the same thing. BUT how many of the bicycles we see on the road are loaded that way? They do not dismiss trail as a mechanism so they are not disagreeing with my contention that it is due to trail on 'real bikes'. They just achieve the 'leaning in' by a different mechanism. Funny thing is that I tried a 'butcher's delivery' bike, once. That had a large load out over the small front wheel. It was a real mother to ride. |
| Sep22-11, 07:30 AM | #47 |
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TU Delft also ran into a conflict between their math and their testing of an actual bicycle regarding capsize speed, I don't know if they've since resolved the issue. Link to link to article, showing image of bicycle: Koo06intro.pdf page 4 of this article includes a graph where the upper limit of the "stable" range is just below 8 m/s = 28.8 kph: Koo06.pdf link to treadmill video where 30 kph is described as "very stable", even though it's greater than the 28.8 kph end of the "stable" speed range from the graph in the artitcle linked to above. My guess is this is due to the fact that the tires are not infinitely thin disk, and when leaned, the fact that the contact patch is on the side of the tire results in a outwards torque that keeps the bike from falling inwards as predicted by the capsize speed shown in the graph. treadmill measurments |
| Sep22-11, 07:34 AM | #48 |
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Is there any more need to 'prove' that gyro forces are irrelevant?
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| Sep22-11, 07:41 AM | #49 |
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Here a more complete explanation of the different theories: |
| Sep22-11, 07:53 AM | #50 |
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| Sep22-11, 08:30 AM | #51 |
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