OCR
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jbriggs444 said:OldYat does not contemplate tracks of non-zero thickness.
sophiecentaur said:Of course not. They do not have tracks.
Lol... carry on.
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jbriggs444 said:OldYat does not contemplate tracks of non-zero thickness.
sophiecentaur said:Of course not. They do not have tracks.
Even that idea introduces problems because the rollers on chains bear on different parts of the sprocket teeth as the chain enters or leaves so the effective radius of the drive changes. This would suggest that there is a change in speed as the non-stretchable chain transitions but, in addition to having a different radius of rotation, the rollers actually move forward and backward, tangentially to compensate because of the profile of the teeth. Putting it another way, there is a radial component as well as a tangential component of roller velocity as it feeds onto and off the chain. So nothing is easy.Tom.G said:Hey guys. Can you all settle on a simplification of considering the 'Track' to be a chain and the 'Lugs' retaining the same attachment as in the OP?
That might bypass getting tangled up in side issues.
The simple model being described contemplates a belt that stretches without thinning [or compresses without thickening]. That model requires a sudden change in density and in speed. However, that is much ado about nothing. Even if we apply a realistic condition of thinning, it is still the case that the outer surface of the belt moves more rapidly than the inner surface in the region where it is wrapped around the drive wheel. Accordingly, it is a simple fact of the matter that the speed of at least one of the two surfaces will change speed during the transition from flat to curved and back to flat.OldYat47 said:A couple of comments: First, if the belt stretches elastically there is no "sudden change" in thickness. It tapers as it is stretched. On the top section and all the way to where it is in contact with the ground it would be stretched along its entire length by the effects of the drive gear pulling it. Second, I have definitely been trying to describe belts of non-zero thickness. Lastly, I am out of here. This thread is hopeless.
Do the math.OldYat47 said:You guys are a laugh. From very early on I have been talking about forward speed being the same as the tangential velocity of the outer surface of the track. "Requires a sudden change in density and speed"? Sheesh.
OldYat47 said:From very early on I have been talking about forward speed being the same as the tangential velocity of the outer surface of the track.
When track links reach the sprocket they transition from linear motion to rotational motion. This means the outer lug tips change speed and get further apart. When the track leaves the sprocket the reverse happens.OldYat47 said:"Requires a sudden change in density and speed"? Sheesh.
And "sheesh" is supposed to be a valid argument against it? If you do not understand it then don't try to argue against it.OldYat47 said:"Requires a sudden change in density and speed"? Sheesh.
Wheel, yes. Track, no.OldYat47 said:What is the effective radius? It's the distance from the center of rotation to the outside surface of the wheel (or track).
Why do you keep asserting this without any explanation or proof? (And don't say "it's obvious" because it appears that it's only obvious to you.)OldYat47 said:It's the distance from the center of rotation to the outside surface of the wheel (or track).
That is blindingly obvious but the motion of the straight bit of the track is not "rolling", it's linear and the clue is in the word "straight". When it leaves the circumference of the wheel (or joins it) the motion kind of motion changes instantaneously (if the track is totally rigid and the contact with the wheel is truly circular or non-slipping.OldYat47 said:Any physics or mechanical textbook will give the same equations for rolling motion.
Maybe OldYat47 thinks about a snowmobile doing a wheelie, and thus driving on the sprocket!sophiecentaur said:That is blindingly obvious but the motion of the straight bit of the track is not "rolling", it's linear and the clue is in the word "straight".
This obscures the important point that the speed of the outer surface of the track as it lays flat on the ground will not, in general, match the speed of the outer surface of the track as it curves around the drive wheel.OldYat47 said:Note that as a wheel rolls there is always one point that is stationary (on the ground) and one point 180 degrees opposite that is traveling "forward" at twice the vehicle speed.
Correct me if I am wrong. I think you have only posted a ref to one site and the whole of that web page was dealing with wheels and wheeled vehicles - which do not have tracks. You are asking us to extend what's written about wheels and to "imagine" what happens to a track, wrapped around the wheel. That is precisely what you are not doing. You are making assumptions and making assertions on a false basis, rather than following all the arguments that have been put to you.OldYat47 said:Now look at the third sketch in that physics site I referred to.
Perhaps you would give us your thoughts on that.sophiecentaur said:Read the following carefully. You have two drive wheels, driven in perfect sync, with a single chain or gearbox. One has the track going round it and the other is on a flat section [of track] over the ground. Both wheels are going forward at the same speed (bolted to the frame) and both wheels are rotating at the same rate. Is one of them slipping on the track? How does your conjecture fit those conditions?
No. In general, it will not be.OldYat47 said:And yes, the point on the track that is stationary as the track leaves the wheel will be identically the point touching the ground.
It doesn't matter which sprocket you do the wheelie on. If the contact to the ground was on a curved part of the track, where the outer track surface moves faster than the inner, then the thickness would affect the gear ratio. But in reality the contact to the ground is on the straight part, where inner and outer track move at the same speed, which doesn't depend on the track thickness.OldYat47 said:And doing a wheelie would not put the drive gear on the ground.
OldYat47 said:The entire track, every little bit of it that lays on the ground is not moving at all.
OldYat47 said:The entire track, every little bit of it that lays on the ground is not moving at all.
OldYat47 said:The track starts at the top traveling twice vehicle speed and when it reaches the bottom it's speed is zero. You can resolve the tangential velocity into two components, one relative to the ground and one relative to the forward speed of the vehicle.
About the track speeds relative to the ground, sure. About the rest, nope.OCR said:Again, OldYat is correct...
Two good videos. Thanks for finding and posting them. I watched all of both of them and it's actually quite apparent that the visible, outer parts of the track are going faster around the wheels than on the flat sections (more to the point, faster than the vehicle is moving forward). The track treads appear to 'whip round' the end wheels visibly faster than anywhere else. Compared with the wheel radius, the depth of the track appears to be at least 10%. That would imply the rotational speed would be at least 1.1 X the linear speed.OCR said:
My alternative is not to look at the irrelevant parts of the track (over the top) but to look at what happens where the curved section mets the flat section. You clearly have not read my arguments (nor any of the others, I suspect) because you are so convinced of your own. None of us has a problem between talking about velocities relative to the vehicle so why do you keep introducing the fact that the track is actually stationary on the ground. Of course it is.OldYat47 said:What's your alternative?
AT's diagram, above really demands a comment from you, too. Why do you never respond to such 'details'?sophiecentaur said:Read the following carefully. You have two drive wheels, driven in perfect sync, with a single chain or gearbox. One has the track going round it and the other is on a flat section over the ground. Both wheels are going forward at the same speed (bolted to the frame) and both wheels are rotating at the same rate. Is one of them slipping on the track? How does your conjecture fit those conditions?
sophiecentaur said:You are asking us to extend what's written about wheels and to "imagine" what happens to a track, wrapped around the wheel.
Again, OldYat is still correct.....
There is no track flat on the ground between those two wheels and no indication of the thickness that such a track might have. The crux of the... vigorous debate here is on the behavior of the inner and outer surfaces of such a track at or near the boundaries between its curved and its flat segments.OCR said:Help at all... even a little?