Re: Book: Advanced Rider Trainer: The Handbook for Training the Trainer
Posted: Tue Jan 26, 2021 8:54 am
Here's an explanation...
Firstly, MOMENTUM (which is the product of mass x velocity) always wants to go in a straight line. If you were able to throw a cricket ball in space, it would travel in a straight line from the moment you released it. It needs a FORCE to make it change speed or direction. On earth, the ball is subject to the force of gravity which pulls it back to the ground, plus the force generated by wind resistance which slows it down. The momentum of the bike is no different - it wants to go straight on, and the rider has to input a force to make the bike change direction.
Secondly, at anything over about 10 mph, road bikes are designed to be STRAIGHT LINE STABLE - remove your hands from the bars, and they'll carry on in a straight line with no input from the rider at all, even if the front wheel hits a bump - the bars will wobble then self-correct*. If you're leaning over when you let go of the bars, the bike will snap UPRIGHT with NO INPUT from the rider. You can see that from some rather odd track crashes - when the rider parts company with the bike, but the bike bounces back upright again... it'll carry on minus rider until the speed drops down to walking pace when it finally falls over. ONLY AT WALKING PACE does the rider need to actively steer in the mild weaves which Horse is talking about. It's easy to try. Get up to 20 mph (you'll need a big empty car park or deserted straight road with a mild camber) ideally in 3rd gear if the bike will do it so you don't get too much engine braking, then simply lift your hands just off the bars. The bike will roll straight until the speed drops down to about 10 mph, then the bike will start to wander, and finally (it's about 6-7 mph on my bikes), it'll threaten to fall over at which point you have to actively steer it. (* Which should tell you most of the instability in a bike travelling at any speed is induced by the rider.)
So the bike's stability in a straight line is a combination of its design and momentum.
Thirdly, momentum acts on the combined Centre of Mass (cCoM) of bike and rider. Very roughly speaking, it's usually about where the back of the tank meets the front of the seat - that means it is around 750 - 800 mm ABOVE the surface of the road.
But - fourthly - the force we apply to get a bike to CHANGE DIRECTION necessarily happens where the tyre touches the road SURFACE.
And this is where it gets interesting.
Moving in a straight line, the cCoM is directly above the line connecting the points where the tyres touch the surface - the bike's mass is balanced directly over the points of contact with the ground.
Imagine what would happen if you stood by a perfectly-balanced bike and pulled a rug out from under the front wheel. If you were standing to the right of the machine, the front wheel would be pulled to the right - and the bike would topple left.
When we steer the front wheel to point to the RIGHT, the force acts on the wheel to pull it to the right - and through it, the forks and the rest of the bike - works at ground level. The mass of the bike meanwhile - acting through the cCoM at the height of the seat - tries to go straight on.
You should be able to see what happens next. With the front wheel steering to the right, the cCoM is no longer directly above the line connecting the wheels, and the bike leans to the left.
Effectively, when we counter-steer, we're pulling the front wheel out from under the cCoM to the right, the moving bike actually topples to the LEFT.
You can try this without riding the bike. Try walking along by placing one foot directly in front of the other - this means you're balancing just like the bike and you should be able to stay upright with no big problem because your CoM is directly above your feet. Now take one more pace but place your left foot to the RIGHT of your other foot - you'll find you lose your balance and your body topples LEFT! It's analogous to the front wheel steering out from under the bike, with the bike toppling the other way.
That's enough to explain the INITIATION of counter-steering - there's actually a bit more to know about what's happening mid-corner and why the bike wants to straighten up again, but the info above is enough to get the bike to ROLL off the vertical and to generate a LEAN angle to get you round a bend.
Although people love to do demos with spinning bicycle wheels to 'prove' that the front wheel is a gyroscope (it is) and because you're forcing the gyroscope to lean it steers the bike (it doesn't - gyroscopic precession is insignificant and IIRC Tony Foale calculated it was around 5% of the forces operating on the front wheel), it's almost entirely down to straight-line momentum, and the steered wheel causing the bike to topple sideways.
Firstly, MOMENTUM (which is the product of mass x velocity) always wants to go in a straight line. If you were able to throw a cricket ball in space, it would travel in a straight line from the moment you released it. It needs a FORCE to make it change speed or direction. On earth, the ball is subject to the force of gravity which pulls it back to the ground, plus the force generated by wind resistance which slows it down. The momentum of the bike is no different - it wants to go straight on, and the rider has to input a force to make the bike change direction.
Secondly, at anything over about 10 mph, road bikes are designed to be STRAIGHT LINE STABLE - remove your hands from the bars, and they'll carry on in a straight line with no input from the rider at all, even if the front wheel hits a bump - the bars will wobble then self-correct*. If you're leaning over when you let go of the bars, the bike will snap UPRIGHT with NO INPUT from the rider. You can see that from some rather odd track crashes - when the rider parts company with the bike, but the bike bounces back upright again... it'll carry on minus rider until the speed drops down to walking pace when it finally falls over. ONLY AT WALKING PACE does the rider need to actively steer in the mild weaves which Horse is talking about. It's easy to try. Get up to 20 mph (you'll need a big empty car park or deserted straight road with a mild camber) ideally in 3rd gear if the bike will do it so you don't get too much engine braking, then simply lift your hands just off the bars. The bike will roll straight until the speed drops down to about 10 mph, then the bike will start to wander, and finally (it's about 6-7 mph on my bikes), it'll threaten to fall over at which point you have to actively steer it. (* Which should tell you most of the instability in a bike travelling at any speed is induced by the rider.)
So the bike's stability in a straight line is a combination of its design and momentum.
Thirdly, momentum acts on the combined Centre of Mass (cCoM) of bike and rider. Very roughly speaking, it's usually about where the back of the tank meets the front of the seat - that means it is around 750 - 800 mm ABOVE the surface of the road.
But - fourthly - the force we apply to get a bike to CHANGE DIRECTION necessarily happens where the tyre touches the road SURFACE.
And this is where it gets interesting.
Moving in a straight line, the cCoM is directly above the line connecting the points where the tyres touch the surface - the bike's mass is balanced directly over the points of contact with the ground.
Imagine what would happen if you stood by a perfectly-balanced bike and pulled a rug out from under the front wheel. If you were standing to the right of the machine, the front wheel would be pulled to the right - and the bike would topple left.
When we steer the front wheel to point to the RIGHT, the force acts on the wheel to pull it to the right - and through it, the forks and the rest of the bike - works at ground level. The mass of the bike meanwhile - acting through the cCoM at the height of the seat - tries to go straight on.
You should be able to see what happens next. With the front wheel steering to the right, the cCoM is no longer directly above the line connecting the wheels, and the bike leans to the left.
Effectively, when we counter-steer, we're pulling the front wheel out from under the cCoM to the right, the moving bike actually topples to the LEFT.
You can try this without riding the bike. Try walking along by placing one foot directly in front of the other - this means you're balancing just like the bike and you should be able to stay upright with no big problem because your CoM is directly above your feet. Now take one more pace but place your left foot to the RIGHT of your other foot - you'll find you lose your balance and your body topples LEFT! It's analogous to the front wheel steering out from under the bike, with the bike toppling the other way.
That's enough to explain the INITIATION of counter-steering - there's actually a bit more to know about what's happening mid-corner and why the bike wants to straighten up again, but the info above is enough to get the bike to ROLL off the vertical and to generate a LEAN angle to get you round a bend.
Although people love to do demos with spinning bicycle wheels to 'prove' that the front wheel is a gyroscope (it is) and because you're forcing the gyroscope to lean it steers the bike (it doesn't - gyroscopic precession is insignificant and IIRC Tony Foale calculated it was around 5% of the forces operating on the front wheel), it's almost entirely down to straight-line momentum, and the steered wheel causing the bike to topple sideways.