ESponge2000 said:
If there is a moving platform underneath a car and the car is in neutral, and the car engine is off and not operating at all … it will appear relative to the moving floor that the car is in motion … now if the moving floor is what’s being powered by an electric current , not the car
And then the moving floor is suddenly shut off with a rapid de acceleration, and I’m inside the car , is it true or not true that i would see the illusion of the car coming to a rapid stop, the wheels of the car forced to stop spinning round and round , but I would not need a seatbelt because my inertia was and remains at rest with the earth and it’s the moving platform beneath the car that changed inertial frames ?
My understanding is yes in this situation there would not be a change in inertia inside the car but yet if i am staring at the moving floor as if its a rest frame , at constant velocity I will get the illusion the car could be in operation but once the platform turns off i won’t detect this change in inertia which is very important as it illustrates the point that while velocity is relative , help me understand how a change in inertia isn’t an absolute ? In this exercise you can distinguish it by the need for a seatbelt vs not
The relevant concept is that of a
non-inertial reference frame. In Newtonian physics, Newton's laws hold in any inertial reference frame. But, in a non-inertial frame, Newton's laws do not hold - unless you include one or more
fictitious forces.
In an inertial frame, an object only accelerates if acted on by an unbalanced (real) force. In a non-inertial frame, an object may accelerate when acted on by no real forces. I.e. Newton's first law does not hold.
When analysing motion you must know, therefore, whether you are using an inertial or non-inertial reference frame.
This also holds in special relativity, although dealing with non-inertial frames is trickier than it is in Newtonian physics.
In GR, there are no global inertial reference frames. You can never simplify things to the same extent that you can in Newtonian physics or Special Relativity.
For example, in GR, in the reference frame of the Sun, the Earth moves in a circular orbit (which implies kinematic, centripetal acceleration). However, there is no real centripetal force acting on the Earth. This shows that the Sun's reference frame is non-inertial.
There is no way to explain this using Newtonian physics - which would require a force to keep the Earth in orbit. There is no point, therefore, in starting to study GR with Newton's laws (or even SR) as your guiding principle. GR is a different ball-game altogether.