B A contradiction of the equivalence principle?

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Larger masses do experience a greater gravitational force, but they also have more inertia, leading to the same acceleration for all objects in free fall near Earth's surface, regardless of mass. This principle is rooted in Newton's laws, where the mass cancels out in the equations for gravitational force and acceleration. The equivalence principle, which states that gravitational mass and inertial mass are equivalent, applies in local contexts where tidal effects are negligible. Therefore, in the hypothetical scenario of Mercury and the Moon falling towards Earth from the same distance, both would accelerate at the same rate, not fall at different speeds. Understanding this concept is crucial for grasping the fundamentals of gravitational physics.
  • #51
PeroK said:
You need to take a step back and think about what you are asking. Here's one reason: objects have a physical size. The above equation refers to the distance ##r## between the centres of mass. A physically larger object will hit the ground first (if dropped in a vacuum chamber). It's much more about size than mass.

Shape also matters, as the above equation ##F = \frac{GMm}{r^2}## only applies to hypothetical point masses and perfect spheres.

For small objects, size and shape are many orders of magnitude more important than mass.
OK consider that both objects have the same size but different masses. then would they both reach the earth's surface at the same time?
 
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  • #52
PeroK said:
If you dropped an object of mass 1kg from the same distance as the Moon, then it would take a certain time to fall to half that distance.

If the Moon were released from rest at the same distance from Earth, then:

a) It would move half that distance in less time than the 1kg object.
b) The Earth would also have moved significantly, so the overall distance between the Moon and the Earth would be less than half the original distance at that time.
This way of describing it might be confusing since there are multiple "distances" being mixed together.

Let's try a simpler scenario: two equal masses ##m## starting from rest separated by a distance ##r##, using a barycentric coordinate system, so the origin of coordinates is halfway between the masses. This spatial origin is also where the masses will collide with each other, ending the experiment. The question is, what time will it take for them to collide?

Since the situation is symmetric, we can just consider one mass. Its acceleration, from previously given equations, is ##G m / r^2##. Notice that this acceleration depends on the mass ##m## (since both masses are identical and the mass appears twice in the gravitational force formula). So the acceleration of each mass towards the barycenter will be larger the larger the mass ##m## is. That means the time to collision, which is the time for each mass to move half the distance between them, will be shorter the larger the mass ##m## is. This last statement is independent of our choice of coordinates.

If we look at this in coordinates centered on the other mass, the coordinate acceleration at the start does not change, it's still ##G m / r^2##; but now there is a correction that has to be added because the origin of these new coordinates is itself accelerating towards the barycenter. In other words, these coordinates are not inertial, unlike the barycentric ones which are. So the starting coordinate acceleration alone does not determine the coordinate trajectory in this frame, as it does in the barycentric frame.

The qualitative logic above does not change when the two masses are unequal, as for the Earth and the Moon vs. the Earth and a 1 kg mass starting at the same distance as the Moon, but of course the numerical details will be different.
 
  • #53
jeff einstein said:
ok then lets consider that we drop these objects at different times. so in theory the object with more mass will reach the ground first (this was agreed by you earlier).
I didn't agree that. I said the Moon would fall faster than a ##1kg## mass.
jeff einstein said:
so doesn't contradict the idea that all masses reach the earth's surface at the same time when held at the same distance. how does this make sense
Every statement has a set of hypotheses under which it is valid. It does not apply if the hypotheses are not met. This often doesn't matter. But if you dig deep enough, the hypotheses on which the statement is based fail.
jeff einstein said:
Either the theory is wrong
It's not wrong. It has what's called a domain of applicability. Also, almost all theories are approximations in some respect. For example, the Earth is not a perfect sphere, it's spinning and its s mass is not constant over time.

I'm trying to get you to think that the theory is approximate in ways that are more significant than the immeasurable motion of the Earth. Like considering the size and shape of objects and not just their mass.
 
  • #54
how about when i talk just about mass
 
  • #55
PeroK said:
I didn't agree that. I said the Moon would fall faster than a ##1kg## mass.
But isn't that still two different masses Here we can see a large difference between this action but for masses with less weight such as 1.5kg and 1kg this should also be true
Shouldn't it?
 
  • #56
jeff einstein said:
how about when i talk just about mass
I think we have exhausted this topic.
 
  • #57
so you give up sir? and i can go around with my "unproved" misunderstanding on this topic
 
  • #58
jeff einstein said:
so you give up sir? and i can go around with my "unproved" misunderstanding on this topic
That's your decision.
 
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  • #59
jeff einstein said:
so doesn't contradict the idea that all masses reach the earth's surface at the same time when held at the same distance
I have never seen that claim. All masses accelerate at the same rate when at the same distance from earth. That is a different claim than the claim that they reach the ground at the same time.

I think you are just misunderstanding the claim.
 
  • #60
so maybe I understood it wrong but in reality, different masses dropped at a certain height do reach the ground at different times?
 
  • #61
jeff einstein said:
different masses dropped at a certain height do reach the ground at different times?
Yes. Different masses accelerate the same in the Earth’s field. But the Earth accelerates differently in different masses fields.
 
  • #62
PeterDonis said:
No, this is wrong. ##F = ma## applies separately to the two masses, so you have ##F = m_1 a_1## and ##F = m_2 a_2##. Then you can solve for ##a_1## and ##a_2##.

Ahhh..... thanks, I thought it looked too easy. So, closing acceleration is . . . okay, given the length of this thread, I find the math answer to the OP's question hilariously simple.
 
  • #63
yes sir the maths is simple but the thought is hard
 
  • #64
so i can now conclude that all masses accelerate to the earth at the same rate but different masses reach the ground at different times when held at a particular distance. am i right @Dale and @PeroK sir?
 
  • #65
actually, i have high respect for you all as you have so much patience... you are probably way more experienced than me at physics and you actually took your time to explain a misunderstood topic to a confused school boy. thank you very much!!!
 
  • #66
jeff einstein said:
so i can now conclude that all masses accelerate to the earth at the same rate but different masses reach the ground at different times when held at a particular distance. am i right @Dale and @PeroK sir?
just clarify this then i am done
 
  • #67
jeff einstein said:
so i can now conclude that all masses accelerate to the earth at the same rate but different masses reach the ground at different times when held at a particular distance.
I understand the math involved though I didn't show it nor give you an answer, but your explanation of your understanding is self-contradictory and makes no sense, so we have no way of knowing if you actually "get it".

Care to reciprocate the massive amount of time forum members have put into your query under your conditions, and show us the three lines of math involved ? to prove that you actually do understand the answer to whatever your question was in the first place. Or, was your purpose more along the lines of manipulation.
 
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  • #68
To recap:
  1. Objects of different masses will all fall to Earth at the same rate (ignoring air resistance) - with the proviso that the objects' masses are insignificant in comparison to Earth's mass.
  2. For objects whose mass is a non-insignificant fraction of Earth's, one must take into account the object's own gravitational effect on Earth.
Technically, these are not two distinct cases. Case 1 is an arbitrary simplification of Case 2, wherein we choose to ignore the miniscule effect of a small object's gravitational influence on the outcome. Which is why you have likely encountered both forms of solution in-the-wild.(Right?)
 
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  • #69
PeroK said:
Like considering the size and shape of objects and not just their mass.
I think this is a distraction from the main point of the thread. At the very least, I think we should get clear about the simple case, where the masses are moving in vacuum and tidal effects are ignored, before trying to add complications.
 
  • #70
jeff einstein said:
just clarify this then i am done
Please read my post #52.
 
  • #71
jeff einstein said:
different masses dropped at a certain height do reach the ground at different times?
Again, read my post #52.
 
  • #72
Here's my answer. We drop a 1 kg mass and 2 kg mass from 10m above the Earth's surface. Making some basic assumptions ... The 2kg mass hits the ground at time ##t_2##. After time ##t_2##, when the experiment is repeated with the 1kg mass, that mass is still ##1 \times 10^{-24} m## above the ground. It takes a further ##1 \times 10^{-25} s## for the ##1 kg## object to hit the ground.

A measurement of ##1 \times 10^{-24} m## in the position of an object is outside the domain of applicability of classical physics.

To test the statement, we need a theory that is applicable on this scale.
 
  • #73
jeff einstein said:
so you give up sir? and i can go around with my "unproved" misunderstanding on this topic
No. You need to think more carefully about exactly what the different claims involved mean. I am hoping that my post #52 will help. At the very least, it should give you more of a framework for thinking about the problem.
 
  • #74
jeff einstein said:
so i can now conclude that all masses accelerate to the earth at the same rate but different masses reach the ground at different times when held at a particular distance. am i right @Dale and @PeroK sir?
Yes.
 
  • #75
PeroK said:
Making some basic assumptions ... The 2kg mass hits the ground at time ##t_2##. After time ##t_2##, when the experiment is repeated with the 1kg mass, that mass is still ##1 \times 10^{-24} m## above the ground. It takes a further ##1 \times 10^{-25} s## for the ##1 kg## object to hit the ground.
This is the part that you can't just handwave in this scenario. You need to show the OP the actual math, since he is only in 11th grade and probably has not had the opportunity to work such problems in detail. I know he said originally that he wasn't interested in the math, but the fact remains that the math is there and is what we all are relying on in making our posts, and without it we're just asking the OP to take claims on our authority, which he is quite justified in refusing to do, since no one should ever take scientific claims as true just on someone else's authority.

I gave the math for a simpler example in post #52, but the basic ideas I gave there are applicable to this scenario.
 
  • #76
PeterDonis said:
I gave the math for a simpler example in post #52, but the basic ideas I gave there are applicable to this scenario.
I missed post #52 entirely in the wave of posts from the OP.
 
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  • #77
##F = \frac{Gm_1m_2}{r^2} \Rightarrow##
##a_1+a_2 = \frac{G(m_1m_2)}{r^2m_1} + \frac{G(m_1m_2)}{r^2m_2} = \frac{G(m_1 + m_2)}{r^2}\Rightarrow##
##a \propto m_1 + m_2##

[edit: note that ##a## is the total of the closing accelerations ##a_1## and ##a_2## and that the calculations were performed within the framework necessitated by same, ie: it ain't sloppy math]
 
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  • #78
hmmm27 said:
##F = \frac{Gm_1m_2}{r^2} \Rightarrow##
##a_1+a_2 = \frac{G(m_1m_2)}{r^2m_1} + \frac{G(m_1m_2)}{r^2m_2} = \frac{G(m_1 + m_2)}{r^2}\Rightarrow##
##a \propto m_1 + m_2##
The accelerations will be of opposite signs (assuming we're just looking at radial motion, as we are in this thread, otherwise we have to do full vector addition), so there should be a minus sign in your last equation, not a plus sign.

Also, your ##\alpha## (corrected as above) is the acceleration of one mass in a non-inertial frame in which the other mass is at rest. That makes its physical interpretation more complicated. The case where the motion of both masses is significant is best handled, IMO, in a barycentric frame, as I did (for the case of equal masses) in post #52.
 
  • #79
I probably have a misconception but my physics teachers say that when an object is dropped at a certain height both objects "pull" on each other with the same "force" meaning that even the very very tiny amount of gravitational force the object has compared to the earth has an effect in the collision. all I am asking is are we ignoring the object's gravity cause it's too small? That is why I initially used larger masses such as mercury and the moon which have their own gravity that is noticeable.
 
  • #80
jeff einstein said:
my physics teachers say that when an object is dropped at a certain height both objects "pull" on each other with the same "force" meaning that even the very very tiny amount of gravitational force the object has compared to the earth has an effect in the collision
The force on both objects has the same magnitude, which depends on the product of the masses, so yes, the mass of both objects affects the magnitude of the force.

The acceleration of both objects, however, is not the same, because it is the force divided by the mass of the object. If one object is very, very, very much more massive than the other (as with the Earth and an ordinary object like a rock, or you), then that object's acceleration is so miniscule as to not be observable, and can be ignored. But if the masses of the objects are not that different (as with the Earth and Mercury or the Moon), then the acceleration of both has to be taken into account. That is what various posts in this thread, including my post #52, have been trying to explain.
 
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  • #81
jeff einstein said:
objects "pull" on each other with the same "force" meaning that even the very very tiny amount of gravitational force the object has compared to the earth has an effect in the collision. all I am asking is are we ignoring the object's gravity cause it's too small?
Yes.
 
  • #82
jeff einstein said:
OK, maybe I am wrong about the theory of equivalence. what I actually meant was the idea that all masses fall to the earth at the same velocity. and I have been asked about if know the equation relating to this, Yes I do but I clearly mentioned that I do not want equations used for this doubt clearance. after all, I want to clarify one thing, Mercury (larger mass relative to the moon) "would fall to the earth" faster than the moon (smaller mass) both positioned at an equal distance, am I right?

There is a caveat here in that these masses are large enough to make the Earth’s acceleration significant, and the Earth’s acceleration is not the same in the two cases. There is no problem dealing with that, but I think that just clouds your issue (particularly if you don’t like math) and we should stick with comparing bowling balls and feathers so we can ignore the Earth’s response.

To be fair (I almost hate to do this) I think I’ll have to explain. To be more precise, at the moment the two cases are at the same distance from the Earth they both experience the same acceleration (relative to the fixed stars, say). As described in previous posts, both the Force and the inertia are proportional to mass and the mass cancels. So, in that sense, they do not fall at different rates.

However, the Earth is also being pulled and has its own significant acceleration. The Earth’s acceleration is different in the two cases, so Mercury would get to the Earth sooner. So in that sense you could say it falls faster.

Or, to put it another way, in center of mass coordinates the acceleration of the second mass is not independent of the second mass. However, the dependence is $$ \left( \frac {m_1} {m_1 + m_2} \right) ^2 $$ so when m1 is significantly greater than m2 this quickly becomes 1.
 
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  • #83
Cutter Ketch said:
...the Earth’s acceleration is not the same in the two cases ... I think that just clouds your issue ... and we should stick with comparing bowling balls and feathers so we can ignore the Earth’s response.
On the contrary; it is the very thing the OP is now asking about, if you follow their most recent posts.
 
  • #84
Cutter Ketch said:
There is a caveat here in that these masses are large enough to make the Earth’s acceleration significant, and the Earth’s acceleration is not the same in the two cases. There is no problem dealing with that, but I think that just clouds your issue (particularly if you don’t like math) and we should stick with comparing bowling balls and feathers so we can ignore the Earth’s response.

To be fair (I almost hate to do this) I think I’ll have to explain. To be more precise, at the moment the two cases are at the same distance from the Earth they both experience the same acceleration (relative to the fixed stars, say). As described in previous posts, both the Force and the inertia are proportional to mass and the mass cancels. So, in that sense, they do not fall at different rates.

However, the Earth is also being pulled and has its own significant acceleration. The Earth’s acceleration is different in the two cases, so Mercury would get to the Earth sooner. So in that sense you could say it falls faster.

Or, to put it another way, in center of mass coordinates the acceleration of the second mass is not independent of the second mass. However, the dependence is $$ \left( \frac {m_1} {m_1 + m_2} \right) ^2 $$ so when m1 is significantly greater than m2 this quickly becomes 1.
i understand this part really well and you have now further solidified my understanding by confirming it but even if this effect was very very very very microscopic I say that larger masses accelerate either slower or faster compared to smaller masses. I say slower or faster because I have a reason let me post an image just wait
 
  • #85
In the first case, both masses are the same and accelerate toward each other at the same rate. Now in cases 2 and 3, I have reduced the mass (m1), as this happens point of collision moves towards the greater mass. Now let's consider that all 3 collisions take the exact same time for collision. the distance between the objects in all three cases is the same. Now looking specifically at cases 2 and 3 we can see that the m1 object has a larger distance to cover compared to the m2 object. Because of this, I conclude that acceleration has to be different in both cases. Yes, I have kind of magnified this idea in the thought experiment, but even though (if this effect is true) this effect is very very insignificant. it's still present. Yes, this may not affect physical experiments at large, but I still persist that the effect is present.

PS: If this thought experiment is false feel free to challenge
me.
 
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  • #86
reference image:
E3F077FB-678F-49C1-A911-7730621462A6 (1).jpeg
 
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  • #87
Your diagram only shows two cases. 🤔
 
  • #88
jeff einstein said:
Now let's consider that all 3 collisions take the exact same time for collision. the distance between the objects in all three cases is the same.
They take different times. The variable mass falls with the same acceleration in each case, but the non-variable mass has a different acceleration in each case. If they start with the same separation then the time will necessarily vary with longer times for slower accelerations of the non-variable mass.
 
  • #89
DaveC426913 said:
Your diagram only shows two cases. 🤔
sorry my bad I had posted the whole writing but sir @Dale said it was hard to read so i cropped the image and I cropped the wrong
 
  • #90
jeff einstein said:
...we can see that the m1 object has a larger distance to cover compared to the m2 object. Because of this, I conclude that acceleration has to be different in both cases.
Yes, you are correct.

You can convert F=ma to a=F/m.

For a given F: If m is small, then a is large. If m is large, then a is small.Looked at another way: Newton's first law says the F is equal and opposite, so
m1a1 = m2a2

And again, if m1 is smaller than m2, then a1 will have to be larger than a2
 
  • #91
here:
E3F077FB-678F-49C1-A911-7730621462A6 (3).jpeg
 
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  • #92
DaveC426913 said:
Yes, you are correct.

You can convert F=ma to a=F/m.

For a given F: If m is small, then a is large. If m is large, then a is small.Looked at another way: Newton's first law says the F is equal and opposite, so
m1a1 = m2a2

And again, if m1 is smaller than m2, then a1 will have to be larger than a2
so sir i was right from the start i have tried to prove my point that different masses have different accelerations when dropped at same height
 
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  • #93
am i right?
 
  • #94
No. Different masses do not have different accelerations.

We have already covered this
 
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  • #95
Jeff, are you even considering the messages you are getting? You respond within seconds and we are covering the same ground over and over and over.
 
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  • #96
DaveC426913 said:
Yes, you are correct.

You can convert F=ma to a=F/m.

For a given F: If m is small, then a is large. If m is large, then a is small.Looked at another way: Newton's first law says the F is equal and opposite, so
m1a1 = m2a2

And again, if m1 is smaller than m2, then a1 will have to be larger than a2
but if this is true....
 
  • #97
disprove this i guess...
 
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  • #98
jeff einstein said:
disprove this i guess...
Sorry, we are now mixing up two things. I may be culpable for that.

Two different masses both being under the influence of the same gravity will have the same acceleration. (1)

But that's not the scenario you have diagrammed, above. The scenario you have diagrammed is about different masses under the influence of different gravity (i.e. each others'). (2)

1694713002286.png
 
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  • #99
jeff einstein said:
but if this is true....
jeff einstein said:
disprove this i guess...
You have been instructed by multiple people over multiple pages carefully explaining the situation. Carefully and repeatedly explaining where your original statements were wrong and also where they were almost right. With multiple corrections from multiple people carefully explaining the physics and the source of the confusion.

Then one single person gives one single confused answer after telling you that they were confused because of a mistaken crop, and immediately you just throw out everything you were taught by all of the previous people?

That shows that you are not seeking to learn, you are just seeking validation.

Thread closed. This topic has been done. Do not re-open, just re-read.
 
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  • #100
PeterDonis said:
The acceleration of both objects, however, is not the same, because it is the force divided by the mass of the object.

I know the topic is closed, and the OP has probably not done enough math yet to understand the full answer, but this is the so-called two-body problem:

https://en.wikipedia.org/wiki/Two-body_problem

I post it to stimulate the study of vector calculus and its applications in the future.

Way back when I studied vector calculus, this important application, interestingly, wasn't covered

Strang's calculus textbook is a good place to learn it:
https://ocw.mit.edu/ans7870/resources/Strang/Edited/Calculus/Calculus.pdf

Thanks
Bill
 
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