A contradiction of the equivalence principle?

In summary, the article discusses a potential contradiction to the equivalence principle, which posits that gravitational and inertial masses are equivalent. It presents findings or theoretical arguments that challenge this principle, suggesting that under certain conditions, the behavior of mass in a gravitational field may not align with the predictions of general relativity. This could have implications for our understanding of gravity and the fundamental laws of physics.
  • #71
jeff einstein said:
different masses dropped at a certain height do reach the ground at different times?
Again, read my post #52.
 
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  • #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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