Ball Thrown Up: Constant Speed Despite Height

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Discussion Overview

The discussion revolves around the behavior of a ball thrown straight up, particularly focusing on the speed of the ball at its highest point and the implications of Newtonian and Einsteinian physics on this scenario. Participants explore concepts related to velocity, reference frames, and the nature of motion in both classical and relativistic contexts.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant asserts that according to Newtonian physics, the ball's speed is zero at the topmost point, while another claims that in Einstein's framework, the ball maintains the same speed it was released with.
  • Another participant clarifies that General Relativity (GR) describes the ball's motion as following a geodesic in space-time, emphasizing the distinction between 4-velocity and 3-velocity, and how the latter depends on the chosen reference frame.
  • It is noted that if an object is placed at the maximum height of the ball, its speed relative to the object is zero when they meet, based on a reference frame fixed to the Earth.
  • A further explanation introduces the concept of a local inertial frame, suggesting that in this frame, both the ball and the object have zero relative speed at the moment they coincide.
  • One participant expresses concern that the notion of zero 4-acceleration may lead to misunderstandings regarding the change in speed of the ball according to relativity.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of speed at the ball's highest point, with no consensus reached on whether the ball's speed is zero or remains constant according to different physical theories.

Contextual Notes

The discussion highlights the complexities of defining velocity in different reference frames and the potential for confusion between 3-velocity and 4-velocity in relativistic contexts. The implications of tidal gravity effects are also mentioned but not fully resolved.

rajeshmarndi
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When a ball is thrown up straight overhead. It just follows the curved space with the speed it is being released and seems as if the ball gradually slows down to zero at the top most and return to earth.

If I'm right, according to Newtonian physics, the ball speed is zero at the top. And according to Einstein physics, the ball speed doesn't slows at all, it travel with the same speed it is being released.

So if an object is placed at the top most height the ball achieve. What impact the object would have with the ball at the top most, with zero speed or the speed it is being released.
 
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rajeshmarndi said:
And according to Einstein physics, the ball speed doesn't slows at all, it travel with the same speed it is being released.

No that isn't true. GR says the ball follows a geodesic of the space-time so that its 4-velocity is constant along its worldline; more precisely the 4-velocity of the ball is parallel transported along the geodesic worldline. But you're talking about the 3-velocity of the ball which is quite different from the 4-velocity. The 3-velocity can only be made sense of relative to some coordinate system or reference frame. If the reference frame is fixed to the Earth, such as in your example, then the 3-velocity of the ball will in fact behave in exactly the same way in both Newtonian gravity and GR, modulo higher order special relativistic effects.
 
rajeshmarndi said:
if an object is placed at the top most height the ball achieve. What impact the object would have with the ball at the top most, with zero speed or the speed it is being released.

Zero speed. As WannabeNewton pointed out, "speed" in the sense you are using the term (3-velocity) can only be defined relative to some coordinate system or reference frame. Since the object placed at the topmost height the ball achieves is at rest relative to the Earth, the obvious reference frame to use is one fixed relative to the Earth, and as WBN said, in this frame the ball's speed is zero when it passes the object.

However, we can also reach the same conclusion regarding the relative speed of the object and the ball when they meet by using a frame in which the ball is at rest. As long as the maximum height the ball reaches is not very large, so that the effects of tidal gravity can be neglected, we can construct a local inertial frame covering the entire experiment, in which the ball is always at rest. In this frame, both the ground and the object at the topmost height the ball achieves are accelerated and follow hyperbolic worldlines; and the hyperbolic worldline of the object is just tangent to the ball's worldline (i.e., to the time axis of the local inertial frame), indicating zero speed in this reference frame, at the instant when the ball reaches the object's height. So in this frame as well, we can derive the correct conclusion that the ball and the object have zero relative speed when they meet.
 

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