A bike with a reverse-spinning wheel
www2.eng.cam.ac.uk
www2.eng.cam.ac.uk
I get that there is some effect other than the gyroscopic action of the wheel (how else could you track-stand, after all), but I don't feel like this device proves or disproves anything.
Also, the "begs the question" and the footnote explaining why it's OK to misue that expression was annoying. (If you have to write a paragraph about why you want to use incorrect English, wouldn't it be easier to just edit the misused construction. "This leads us to ask, ..." Write that, and you save yourself a footnote, and people will think you're not bad at writing. </rant>.)
tau = I*domega/dt
When we have two wheels spinning in opposite directions the torque is tau = I*domega/dt + I*d(-omega)/dt = 0
The gyroscopic effect doesn't actually make it harder to turn a wheel. It's just that if you turn it in the xy-plane, it automatically turns in the direction perpendicular to the push (the yz-plane). When a human is physically turning a wheel he will try to stop that from happening, thus the feeling that it's hard to turn the wheel. Note that in particular the gyroscopic effect does not produce any force in the direction opposite to the pushing force.You have a wheel spinning one way, and say that if you try to turn it clockwise in the xy-plane then it will turn clockwise in the yz-plane because of the gyroscopic effect. If you have a wheel spinning the opposite way, and if you turn it clockwise in the xy-plane then it will turn counterclockwise in the yz-plane because of the gyroscopic effect. Adding the two effects cancels them.
However, two wheels spinning in opposite directions may cancel out other spinning wheel effects.
I've done both the math and the experiment - it's in one of the lectures I give on "Spinning Things".
In short, I believe you to be wrong, and this is based on my personal experiments and calculations. I would be interested to know the basis of your claim.
When computed in detail, gyroscopic stability is really the effect that torque applied in one plane manifests itself as movement in another. The direction of this movement depends on the direction of spin, and they cancel each other out when you have two wheels spinning in opposite directions.
My independent experiments and calculations were done before I read anything formal about it, and it agrees with the work of people who design devices that run on satellites and the ISS. I'd need a lot of convincing that I'm wrong.
This is independent of the other effects that help to keep a bike upright, such as the steering geometry. I have experience of that too, having raced bikes with very small rake, and toured on bikes with a larger rake. The difference is unmistakeable, and unrelated to the gyroscopic issues.
http://www.rc-airplane-world.com/coaxial-rc-helicopters.html
And it sure seemed to have a lot of rotational inertia. If you were right, then I could touch one side of the helicopter slightly and since it has no rotational inertia it would tilt to the side and completely change direction and fly off somewhere into the wall or the floor. This did not happen however, even when I tried to tilt it the helicopter remained horizontal. And please do not tell me that a $50 toy has an active stability system with internal gyros and all the required electronics and super fast servos.
And now that I think of it, I remember that the russians have been making counter rotational helicopters for ages. See for example this one:
http://en.wikipedia.org/wiki/Kamov_Ka-25
How does this helicopter stay horizontally stable in the air and does not fly off on a tangent when tilted by the slightest cross wind? Note that this one was designed in the late 50's before any electronic active stability systems could have been invented.
I don't doubt that your experience of a toy double blade helicopter is that it seems to have a lot of rotational inertia. I am certain that it's not due to the gyroscopic stability of exactly matched counter-rotating blades.
However ...
A helicopter changes direction by using the cyclic setting on its rotors. Then you get more lift from one part of the rotor cycle and less from another. That causes the plane of the rotors to tilt, and then the helicopter goes off in the appropriate direction.
For example, having more lift in the rear portion of the cycle and less in the front means the helicopter gets tipped forward, effectively like lifting one part of a plate. The down-draft now has a significant rearwards component, so the rotors get pushed forward, taking the helicopter with it.
If you then change the cyclic to "flat" so there is identical lift everywhere, the weight of the helicopter dangling from the rotors causes it come come back upright (after swinging a bit)
It's a weird experience sitting in a helicopter when it's doing this, especially if you're mostly accustomed to ordinary aeroplanes.
I don't see any contradiction in any of this, and it really doesn't seem to have any bearing on the fact that contra-rotating disks have no net gyroscopic effect.
Yes.
I asked:
> Which other spinning wheel effects? [other than the gyroscopic effect]
And he replied:
> Precession
To which I replied that precession is not a different effect. I did not mean to imply that precession happens when you have two wheels spinning in opposite directions, in fact I believe it does not because the forces that cause a single spinning wheel to precess cancel out if you have two wheels spinning in opposite directions.
I believe that people who believe otherwise are working on misunderstandings of perceptions. It's nototiously easy to confuse several effects in this. Careful experiments are required with tight controls on error bars, etc.
It's easy to be fooled. Eric Laithwaite is a classic and high profile example:
The result was that counter rotating gyroscopes had no net effect.
The only thing that matters is total angular momentum.
The resistance to being tilted is a _secondary_ effect. The push gets translated into motion at right angles to the push, and this motion gets translated into push at one more right-angle, exactly countering the original push. For two counter-rotating gyroscopes, this first-stage motion of one is exactly countered by the other, leading to no net effect. Really, truly.
A bike moving forward will self correct to stay up until it loses speed. A bike moving backward will quickly go into a hard turn right or left and fall over. Gyroscopic moments for wheels in both scenarios are the same. The difference is that as a forward-moving bike falls to one side, the front wheel straightens out underneath it. As a backward moving bike (or any bike with a turning rear wheel), starts to fall, the front (now rear) wheel turns further to the side as it falls rather than straightening out, and the bike goes into a very sharp turn and falls.
As an addendum, that's why recumbent bikes stick with a rear drive and front steer, which requires very long chains, rather than driving the front and steering with the rear (which at first blush seems like a much simpler configuration - the pedals are up near the front wheel, and the hands are near the rear).
Also I think the larger effect on your experiemt is the "trail" thing the author mentioned. If you spin the front wheel 180 degrees (possible for some bikes) and try again I think you'll mostly see the reverse result: pushing the bike backwards will let it roll a while, but pushing it forwards will result in immediate crash. But the leaning effect you mention could be important too, I don't know.
Modern automobiles have incorporated rear wheels that turn together with the front wheel (I believe in opposite directions during a turn) in order to decrease the turning circle and improve maneuverability - I'd kill for a bike that has an electro-servo controlled rear wheel that turns to help the biker corner, etc.
If you only steer the front wheels then when the centripetal force is correct for turning the corner, the rotational force is much larger than necessary. This leads to excessive scrubbing of the tires. Making the rear wheels steer slightly in the direction of turn the rotational force is reduced, similarly reducing the scrubbing.
As a side benefit the wheels can be turned in the opposite direction at low speed, increasing the manoeuvrability.
In this next picture, note the seat post (not the sissy bar) is actually inserted into something like a typical headset (where a fork and stem would go on the front of a bicycle) that pivots when the pin on the underside of the frame is removed. http://www.swingbikerider.com/4-24-05%20003.jpg
[1] (sorry, can't find a better reference/illustration with a cursory googleing) http://www.faqs.org/patents/app/20090014981
[2] http://en.wikipedia.org/wiki/Countersteering (this article may not be sufficient for a thorough understanding of countersteering, but it's a good start)
See: http://www.youtube.com/watch?v=Cbfe2_2DDc0
Additionally, stationary trainers like rollers that don't allow for the steerage correction described by the author illustrate how at speed something other than castor angle is assisting in stabilizing the bike.
http://www.youtube.com/watch?v=9gCnBBeV2ws&feature=relat...
I think that proves things a bit better - we stay up on a bike because we learn to notice any slight chance we're falling, and counteract that with steering to bring us back to upright.
Riding lighter wheels has a lot of effect on acceleration and braking. Handling also improves ALOT with lighter wheels.
It also contributes to stability. But you do need to ride faster than this "wuss" (pun intended) moving at snail speed.
Of course this is all subjective (my observation, and the parent's downhilling observation).
Definitely easier to steer lighter wheels regardless of speed.