Macroscopic objects in free-fall

In summary, macroscopic objects in free-fall experience the same gravitational acceleration regardless of their mass, leading to a uniform rate of descent in a vacuum. This phenomenon is a demonstration of the equivalence principle, which states that the effects of gravity are indistinguishable from acceleration. In practical terms, it explains why objects like a feather and a hammer, when dropped in a vacuum, fall at the same rate, countering common misconceptions influenced by air resistance. Understanding this principle is crucial in physics, particularly in fields related to gravity and motion.
  • #1
cianfa72
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Analysis of macroscopic objects in free-fall in gravitational field
Hi,
very basic question. Take an object like a rock or the Earth itself. If we consider their internal constituents, there will be electromagnetic forces acting between them (Newton's 3th law pairs).

From a global perspective if the rock is free from external non-gravitational forces, then it will be in free-fall in gravitational field (i.e. spacetime geometry).

What about the aforementioned internal forces ? If we look at the center of mass (as object’s representative), then the electromagnetic internal forces driving the object’s costituents away from their geodesic paths will not enter into account, I believe.
 
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  • #2
You clearly, and correctly, state that absent any external forces, a macro object will be in a geodesic freefall path in whatever gravitational field it exists in. THEN, you ask if there is some way internal forces could throw then entire object off that path. Do you see the contradiction?
 
  • #3
phinds said:
Do you see the contradiction?
Yes, I see. I was trying to better understand the reason behind it.

Thus, each object’s costituent path through spacetime is not geodesic due to electromagnetic forces acting on it from other constituents (i.e. they have non-zero path curvature). Yet, the motion of object's center of mass is still geodesic (i.e. in free-fall).
 
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  • #4
I have often found that a way to clarify things is to think of extremes. In this case, think of a fairly thin-walled sphere with some thickness and mass, with a heavy rubber highly elastic ball inside. You shake the sphere vigorously, getting the ball slamming back and forth between opposite sides.

Now you let it go in free fall. The ball keeps bouncing and you think, well, heck, it's obviously going to move the sphere off to one side when it hits that side, so the COM of the sphere clearly moves. Yes, it does, BUT ... the ball is also going move (rebound) thus keep the COM of the entire macro object unmoved (well, still following the geodesic).
 
  • #5
cianfa72 said:
each object’s costituent path through spacetime is not geodesic due to electromagnetic forces acting on it from other constituents (i.e. they have non-zero path curvature). Yet, the motion of object's center of mass is still geodesic (i.e. in free-fall).
Yes, that's correct.
 
  • #6
phinds said:
I have often found that a way to clarify things is to think of extremes. In this case, think of a fairly thin-walled sphere with some thickness and mass, with a heavy rubber highly elastic ball inside. You shake the sphere vigorously, getting the ball slamming back and forth between opposite sides.

Now you let it go in free fall. The ball keeps bouncing and you think, well, heck, it's obviously going to move the sphere off to one side when it hits that side, so the COM of the sphere clearly moves. Yes, it does, BUT ... the ball is also going move (rebound) thus keep the COM of the entire macro object unmoved (well, still following the geodesic).
How does the system behave if instead of a massive ball it is a massless light bouncing inside the sphere?
 
  • #7
Hill said:
How does the system behave if instead of a massive ball it is a massless light bouncing inside the sphere?
Why would it be any different?.
 
  • #8
phinds said:
Why would it be any different?.
Where is a center of mass of the system sphere+light?
 
  • #9
Hill said:
Where is a center of mass of the system sphere+light?
Assuming the system is spherically symmetric (i.e., the light inside the sphere is distributed in a spherically symmetric way), the center of mass would be at the geometric center of the sphere.

You seem to be under a misconception that a system containing parts with zero rest mass, like light, cannot have a center of mass. That is not the case.

A better general term would be "center of energy", or even, if we want to take relativistic effects into account, "center of energy-momentum".
 
  • #10
PeterDonis said:
You seem to be under a misconception
I am not and I do not.

PeterDonis said:
A better general term would be "center of energy", or even, if we want to take relativistic effects into account, "center of energy-momentum".
This is what I aim to.

PeterDonis said:
if we want to take relativistic effects into account
This thread is in the Relativity forum.
 
  • #11
Hill said:
I am not and I do not.
Then I am puzzled as to why you highlighted the words "center of mass" in your post #8. Or indeed why you felt it necessary to ask the question you asked in that post at all, since, as @phinds implied in post #7, the answer is the same for any spherically symmetric distribution, no matter what it is composed of.
 
  • #12
If tidal gravity is significant, it is not clear that the center of mass will coincide with the center of gravity.
 
  • #13
jbriggs444 said:
If tidal gravity is significant, it is not clear that the center of mass will coincide with the center of gravity.
How are you defining "center of gravity" in this case?
 
  • #14
jbriggs444 said:
If tidal gravity is significant
In this case, the composition of the body, given that the distribution of energy and momentum is the same, still will not affect the location of the center of mass.
 
  • #15
PeterDonis said:
In this case, the composition of the body, given that the distribution of energy and momentum is the same, still will not affect the location of the center of mass.
You mean the distribution of energy and momentum is the same since spherically symmetric distribution for the "sphere + light" system is assumed.
 
  • #16
cianfa72 said:
You mean the distribution of energy and momentum is the same
Yes.

cianfa72 said:
since spherically symmetric distribution for the "sphere + light" system is assumed.
It is in the original case, but if tidal effects are present, the distribution won't be spherical.
 
  • #17
PeterDonis said:
It is in the original case, but if tidal effects are present, the distribution won't be spherical.
Yet, the Center of Mass (COM) of the system "sphere + light" will follow a geodesic path through spacetime (i.e. a path with zero curvature).
 
  • #18
PeterDonis said:
It is in the original case, but if tidal effects are present, the distribution won't be spherical.
I am confused by your objection. When you assume the cow to be spherical, it is a "done deal". We already assumed the cow to be spherical, knowing that this might not actually be troooo.
 
  • #19
cianfa72 said:
the Center of Mass (COM) of the system "sphere + light" will follow a geodesic path through spacetime (i.e. a path with zero curvature).
Yes.
 
  • #20
hutchphd said:
When you assume the cow to be spherical, it is a "done deal".
No, when you assume the cow to be spherical, you are also (though you might not realize it) assuming that there are no non-negligible tidal effects. So if you want to consider the case where there are non-negligible tidal effects, you can't assume the cow to be spherical.
 
  • #21
Perhhaps I don't understand the term "tidal effects" in this context?
 
  • #22
hutchphd said:
When you assume the cow to be spherical, it is a "done deal". We already assumed the cow to be spherical
Sorry, what is the term cow ?
 
  • #23
hutchphd said:
Perhhaps I don't understand the term "tidal effects" in this context?
If spacetime curvature is small then the spacetime around our internally mirrored ball is flat (or near enough) and the mass distribution will be spherically symmetrical. If the curvature is larger spacetime is no longer near enough flat, and we don't expect the geometry of spacetime inside the ball to be isotropic. That's tidal gravity. The ball will be non-uniformly stressed and (even if its shape is negligibly affected) the light flight time across it will depend on the angular coordinate, so the mass distribution shifts (in general, anyway - you can probably find special cases).
 
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  • #24
cianfa72 said:
Sorry, what is the term cow ?
Google "spherical cow". It's an old joke about physicists' tendancies to build simple models where the maths is tractable but the model is somewhat divorced from reality.
 
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  • #25
Ibix said:
Google "spherical cow". It's an old joke about physicists' tendencies to build simple models where the maths is tractable but the model is somewhat divorced from reality.
:wink:
 
  • #26
Ibix said:
The ball will be non-uniformly stressed
This ain't no spherical cow where I come from.... Thanks for the explain.
 
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  • #27
hutchphd said:
Perhhaps I don't understand the term "tidal effects" in this context?
@Ibix's explanation is correct. The only technical point I would make is that the tidal distortions of objects that he described are due to Weyl curvature.
 
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  • #28
PeterDonis said:
The only technical point I would make is that the tidal distortions of objects that he described are due to Weyl curvature.
Such a Weyl curvature/tensor describes how the shape of a body is distorted due to spacetime curvature (i.e. geodesic deviation).

My point is: Can electromagnetic forces between body's constituents cope with those "tidal forces" inside the body ?
 
  • #29
cianfa72 said:
My point is: Can electromagnetic forces between body's constituents cope with those "tidal forces" ?
Are you being torn apart by the non-zero tidal force on your body now? If not, then yes they can cope in at least some circumstances. However, extreme tidal forces can overwhelm them - a close orbit over a neutron star might be fatal to a human and you would certainly be killed this way short of the singularity in a black hole. If you search the forum for "ouch radius" (Wheeler's term) you will find some order-of-magnitude discussion.
 
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  • #30
cianfa72 said:
Such a Weyl curvature/tensor describes how the shape of a body is distorted due to spacetime curvature (i.e. geodesic deviation).
More precisely, it describes how the shape of the body is distorted in the absence of any internal forces, i.e., if the body's atoms follow the geodesic paths that the Weyl curvature dictates. Weyl curvature is geodesic deviation.

cianfa72 said:
My point is: Can electromagnetic forces between body's constituents cope with those "tidal forces" inside the body ?
Internal forces inside the body will prevent the body's atoms from following the geodesic paths that the Weyl curvature dictates. Instead they will follow non-geodesic paths. But if the tidal effects are non-negligible, those non-geodesic paths will still result in a shape of the body that is different from what its shape would have been in flat spacetime in the absence of any geodesic deviation (i.e., spacetime curvature).
 
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  • #31
PeterDonis said:
But if the tidal effects are non-negligible, those non-geodesic paths will still result in a shape of the body that is different from what its shape would have been in flat spacetime in the absence of any geodesic deviation (i.e., spacetime curvature).
However, as you highlighted before, even in this case the body's COM continues to follow a geodesic path in free-fall.
 
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  • #32
cianfa72 said:
as you highlighted before, even in this case the body's COM continues to follow a geodesic path in free-fall.
Yes.
 

FAQ: Macroscopic objects in free-fall

What is free-fall?

Free-fall is the motion of a body where gravity is the only force acting upon it. In the absence of air resistance, all objects in free-fall near the Earth's surface accelerate downwards at approximately 9.81 m/s², regardless of their mass.

Do all objects fall at the same rate in free-fall?

Yes, in the absence of air resistance, all objects fall at the same rate in free-fall. This is due to the uniform acceleration due to gravity, which is approximately 9.81 m/s² near the Earth's surface. This principle was famously demonstrated by Galileo.

How does air resistance affect free-fall?

Air resistance opposes the motion of objects through the air and can significantly affect the rate at which they fall. Lighter objects with larger surface areas experience more air resistance and fall slower compared to denser objects with smaller surface areas. In the presence of air resistance, objects reach a terminal velocity where the force of gravity is balanced by the drag force.

What is terminal velocity?

Terminal velocity is the constant speed that a freely falling object eventually reaches when the resistance of the medium through which it is falling prevents further acceleration. At this point, the downward force of gravity is balanced by the upward force of air resistance.

Can free-fall occur in a vacuum?

Yes, free-fall can occur in a vacuum. In a vacuum, there is no air resistance, so objects fall purely under the influence of gravity. This means that all objects, regardless of their mass or shape, will fall at the same rate. This was demonstrated by the Apollo 15 astronauts on the Moon, where a feather and a hammer were dropped simultaneously and hit the ground at the same time.

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