Hiya Rui~
Just a quick question, 'cos this reminded me of something some people were talking about in my class earlier this year: In the non-inertial frame of reference, if the ball is dropped, how come it's a parabolic path (not diagonally linear)?
I eventually taught myself how this works by combining both physics and maths together (although mostly still physics). You're pretty capable so I'll let you try to decipher it, but come back if you need further help
(It's kinda weird to be fair - I visualised it all in my head in a matter of seconds but an explanation takes ages)
The idea is to use projectile motion principles. Pretend that you are about to throw a ball. Whilst the ball is in your hand, you have full control of its motion. However, at the instant the ball leaves your hand, it becomes a projectile.
The point of this, is that at the instant the ball leaves your hand, that's when you can
guarantee that its horizontal velocity is constant. When it was in your hand, you could literally just move the ball back and forth, and that's obviously not a constant horizontal velocity.
Back to relativity.
Pretend we are in an inertial frame of reference first. Suppose you're travelling at some velocity (for visual purposes, let's consider small velocities such as 20ms
-1). Additionally, first suppose that the ball is still in your hand. Then it's obviously travelling at 20ms
-1 with you. Then suppose you release the ball. The ball is in the same inertial frame of reference as before you left it; it's also travelling at 20ms
-1. Hence because both you and the ball are travelling at 20ms
-1, you see it drop vertically.
But why is it, that when you drop the ball, it's still "moving at 20ms
-1"? (Note that I'm trying to keep away from Einsteinian physics here; I'm kinda using Newtonian physics).
Consider a stationary observer watching you travel at 20ms
-1. To him, it appears as though the ball already had an initial velocity of 20ms
-1! You were holding the ball at 20ms
-1 and that's what he saw, but the instant you let go of the ball you basically released it AT horizontal velocity 20ms
-1. So the observer can actually confirm that once the ball is dropped, you are travelling at the same speed as with the ball.
Now for the non-inertial frame of reference.
Once again, you start off by holding the ball still. Except this time you're accelerating. Acceleration is indeed what's going to play a key role here.
Suppose you start accelerating from, idk, at rest. You accelerate from being at rest (at some magnitude) all the way up to 20ms
-1, and THEN you drop the ball. This is where the analogy from earlier comes into play.
When you were accelerating, you had full control of the velocity of the ball. So if you were accelerating, the ball accelerated with you. But once you dropped the ball, it isn't with you anymore; you lost control over the ball! The ball was released when it acquired a velocity of 20ms
-1, so because it's no longer affected by anything (i.e. your hand went away) it now travels by 20ms
-1 by itself.
But whilst the ball is travelling at 20ms
-1 by itself now, what are you doing? You're still accelerating! Because you're getting
faster than 20ms
-1 you start seeing the ball 'lag behind' you now.
The point, is that once you let go of the ball, it formed
its own new INERTIAL frame of reference. You remain as a non-inertial frame of reference because you're accelerating, but nothing drives the ball into accelerating anymore so it's now in an inertial frame. This is also what the stationary observer would see - you're getting faster but the ball appears to stay at the same speed.