Timeline for Hinged Rod end point centripetal acceleration/ tangential acceleration
Current License: CC BY-SA 4.0
6 events
| when toggle format | what | by | license | comment | |
|---|---|---|---|---|---|
| Dec 17, 2018 at 12:37 | vote | accept | delivosa | ||
| Dec 17, 2018 at 12:35 | comment | added | user196418 | At the instant omega = 0, centripetal acc = 0. From my point of view the constraint of the hinge makes it all together illegal to not move in a circle (once motion is set up). | |
| Dec 17, 2018 at 12:34 | comment | added | user196418 | You seem to be creating a scenario where something moves and dosen't move at the same time. See the other answer provided by melp. At the instant you apply a force you create an instantaneous rate of change for v, a change of state. Motion is continuous and you cannot separate the "instant" from neighboring instants. | |
| Dec 17, 2018 at 12:13 | comment | added | delivosa | How can the situation of a resting point and a point that is already moving in a circle be the same? | |
| Dec 17, 2018 at 12:05 | comment | added | delivosa | But at the instant that the force applies it isn't moving in a circle, it is at rest. | |
| Dec 17, 2018 at 12:00 | history | answered | user196418 | CC BY-SA 4.0 |