Time to impact in freefall: mass dependant?

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Discussion Overview

The discussion revolves around the question of whether the time to impact for objects in freefall is dependent on their mass, particularly in the context of classical mechanics and gravitational interactions. Participants explore the implications of mass on the acceleration of both the falling object and the Earth, as well as the assumptions made in typical physics problems.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that while the Earth accelerates all objects equally, the objects themselves do not accelerate the Earth equally, suggesting that heavier objects will have a different time to impact compared to lighter ones.
  • There is a discussion about the assumption of a "fixed" Earth in classical mechanics, with some arguing that this assumption breaks down when the mass of the falling object is significant relative to the Earth's mass.
  • One participant raises the concern that if a very heavy object is dropped, the Earth may not act as a rigid body, and different parts of the Earth could move different distances due to tidal forces.
  • Another point made is that the dynamics of how the Earth responds to the gravitational pull of a falling mass must be considered, as it complicates the calculation of impact time.
  • Some participants acknowledge differing simplifying assumptions in their arguments, indicating a level of agreement on the complexity of the problem without reaching a consensus.

Areas of Agreement / Disagreement

Participants express differing views on the impact of mass on the time to impact, with no consensus reached. There is recognition of the complexity introduced by large masses and the need to reconsider standard assumptions in physics.

Contextual Notes

Limitations include the assumptions of a fixed Earth and rigid body dynamics, as well as the potential influence of tidal forces on the Earth's response to falling masses. These factors remain unresolved in the discussion.

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From a thread in engineering:
Me said:
Danger said:
Haven't you ever seen the demonstration where they drop a ball bearing and a feather in an evacutated cylinder? They accelerate identically.
I have. But that isn't what we're talking about. In that case, both objects are so much smaller than the Earth that the difference isn't noticeable. It's so small, in fact, that we cut it out of the equations because the difference gets lost in the significant digits. But that doesn't mean the difference isn't there.

Perhaps a new thread in GP...
My point is this: though the Earth accelerates the feather and the ball bearing equally, the feather and the ball bearing do not accelerate the earth equally. As a result, the time to impact for the ball bearing will be less than for the feather. For objects that small, it may not be noticeable, but it is still there.

To notice it, you really need bigger masses. Any object arbitrarily low in mass will hit the Earth in about two seconds when dropped from 9.8m. But let's say you could drop another Earth from 9.8m above this one. Since each is being accelerated toward the other at 9.8m/s^2, impact would occur in 1s.
 
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russ_watters said:
From a thread in engineering: My point is this: though the Earth accelerates the feather and the ball bearing equally, the feather and the ball bearing do not accelerate the earth equally. As a result, the time to impact for the ball bearing will be less than for the feather. For objects that small, it may not be noticeable, but it is still there.
To notice it, you really need bigger masses. Any object arbitrarily low in mass will hit the Earth in about two seconds when dropped from 9.8m. But let's say you could drop another Earth from 9.8m above this one. Since each is being accelerated toward the other at 9.8m/s^2, impact would occur in 1s.

We have seen something similar like this a few times on here. Perhaps some day we'll have a definitive explanation and put it up as an FAQ or something.

There is an implicit assumption of a "fixed" Earth when we try to explain the drop of an object. What this means is that the center of mass of the whole system is fixed, and fixed right at the center of the earth. The object then is moving, and falls to the Earth (remember, we're dealing with classical mechanics here). Now, in most cases, this is perfectly valid since most objects that we deal with terrestrially is waaaaaaay smaller and lighter than the Earth itself.

Now, as you have alluded to, what happen if the object is larger and of significant fraction of the earth? Then the center of mass of the system would change, and may in fact no longer be right at the center of the earth. When you have two objects such as these, and you let go, the Earth will start moving towards the other object, while the other object will start moving towards the earth. How fast this happens certainly depends on the force of gravity between the two AND where they meet! The latter also explicitly depends on the masses of both of them since this depends on the center of mass.

So two very light objects will have the same acceleration, and travels the same distance to hit the Earth surface, But a VERY heavy object, comparable to the Earth's mass, will have a different distance to travel before it hits the earth, since the Earth is also moving siginificantly towards it.

Zz.
 
Basically, if you are dropping a heavy enough mass that the Earth moves, I have to also question the auxillary assumption that the Earth is acting as a rigid body.

This assumption is being made when one says that the Earth "moves" a certain distance. It's quite likely that different parts of the Earth move a different distance.

There will be significant and time-varying tidal forces on the Earth due to the falling large mass. I assume that the time is being computed when the falling mass reaches the surface of the Earth that's underneath the mass. Since the Earth is probably not holding it's shape, one would have to include all the dynamics of how the Earth responds to the time-varying tidal forces to answer this question.
 
Okay, I see what you were on about. I was indeed referencing the Earth as a fixed gravity source. When given the reality that it can also be accelerated by the gravity of another body, your argument is correct.
There's another factor which would totally screw up the experiment if one of the bodies is extremely massive. The comparison object would be attracted to both it and Earth, and thus would no longer have a normal 1g acceleration.
 
Yeah, we were just using different simplifying assumptions. We're cool - well, I am, anyway... :cool:
 
Roger that.:biggrin:
 
My, what an interesting look at the standard problem! Great job!
 
We've never embraced the KISS principle.:biggrin:
 

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