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But there is friction? so the momentum is not conserved in the horizontal direction?kuruman said:The velocity of the center of mass of the (wheel + stick) system is initially zero. For the center of mass to be moving in the horizontal direction after the stick is horizontal, there must have been a horizontal force that acted (or continues to act) on it. What is that force and where is it coming from?
To fix your LaTeX problem, bracket your expressions between two ## symbols on each side, not just one.
kuruman said:Imagine the wheel riding on two rails with a gap between them that allows the stick to fall through and swing around. What would the motion of the system look like if there is no energy loss?
When people say "rolling without slipping" they mean that the point on the wheel that is in contact with the surface is instantaneously at rest relative to all points on the surface. In other words, the points that are in contact do not move relative to each other. When there is slipping, the points in contact move relative to each other.mattlfang said:sorry, I don't quite understand this "the wheel riding on two rails with a gap between them that allows the stick to fall through and swing around" part? I don't fully understand what this system looks like?
I start to suspect when people say "Rolling Without Slipping", it implies that momentum is conserved (the change to the momentum can be ignored), despite having a frictional force?
kuruman said:When people say "rolling without slipping" they mean that the point on the wheel that is in contact with the surface is instantaneously at rest relative to all points on the surface. In other words, the points that are in contact do not move relative to each other. When there is slipping, the points in contact move relative to each other.
The figure below shows what I am asking you to imagine. In the front view, the stick falls so that its free end moves out of the screen. In the side view, the free end rotates clockwise in the plane of the screen.
View attachment 291923
You cannot ignore friction when you have rolling without slipping. If you put a wheel on a frictionless incline, it will slide down just like a block without rolling. In this case, the angular speed ##\omega## about the axis of the wheel is zero. If the wheel is rolling down without slipping, then and only then the angular speed is related to the speed of the center of mass of the wheel by ##V_{\text{cm}}=\omega~R.## There is also the intermediate case of rolling with slipping in which case ##V_{\text{cm}}<\omega~R.##mattlfang said:Unless "rolling without slipping" usually entails we can ignore the friction?
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