- #1
EngineeringFuture
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- TL;DR Summary
- This is a question about why a rigid body slides horizontally when the only force applied to it is the vertically-acting gravity. The topics explored are mechanics, the relationship between linear and angular momentum, the nature of rigid bodies and their centers of mass, and other related topics.
I hold my identification card on a low-friction surface by one of its edges. I slightly lean it, and it starts to fall. Before it falls over, I place my finger against the card, and this prevents it from falling all the way over. Then, I withdraw my finger without pushing or pulling the card and let the ID-card fall all the way over and flat. Then, once the card has fallen completely flat on the table, something interesting happens: the card starts to move along the table in the direction of the horizontal component of the circular motion it was making. In fact, even if the table is slightly uphill, the card will move along the direction of the horizontal component of the circular motion it was making.
When I look at this from a perspective of Conservation of Momentum, this makes sense. The card still has momentum from gravity making it fall, and this momentum is why it is moving. There doesn't need to be any acceleration to cause the motion of the card because nearly every particle(I don't know if it is pivoting about completely stationary particles on the card or not) comprising the card is already moving in the horizontal direction and will keep moving in the horizontal direction until a force stops it. The center of mass of the card is moving horizontally already and will keep moving horizontally until friction stops it.
However, from the perspective of a rigid body, it doesn't make sense that the card as a whole accelerates simply because it stops rotating. Gravity acts vertically on the card. There are no other external forces applied to the card. Angular momentum can't be converted to linear momentum. How should I view the linear acceleration of the card once it stops falling?
When I look at this from a perspective of Conservation of Momentum, this makes sense. The card still has momentum from gravity making it fall, and this momentum is why it is moving. There doesn't need to be any acceleration to cause the motion of the card because nearly every particle(I don't know if it is pivoting about completely stationary particles on the card or not) comprising the card is already moving in the horizontal direction and will keep moving in the horizontal direction until a force stops it. The center of mass of the card is moving horizontally already and will keep moving horizontally until friction stops it.
However, from the perspective of a rigid body, it doesn't make sense that the card as a whole accelerates simply because it stops rotating. Gravity acts vertically on the card. There are no other external forces applied to the card. Angular momentum can't be converted to linear momentum. How should I view the linear acceleration of the card once it stops falling?