Time of free fall does depend on mass

In summary: The universality of free fall is always true. The time of free fall is affected by the mass of both bodies.The acceleration of body A is affected only by the mass of body B, and the acceleration of body B is affected only by the mass of body A.If the mass of free falling body A is changed, it's acceleration will not change, but the time of free fall will change.If I'm understanding the op post correctly you may find the above statements confusing or even contradictory, but they are all true.The statements are all true, but they are not always true. For example, if body A has more mass then body B, the time of free fall will be shorter for body
  • #1
parshyaa
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Months ago I have seen walter lewins first lecture on dimensions, there he made a comment that scientist are trying to prove that time taken to reach ground when a object is dropped does depends on mass (in small amount) but it depends on mass, how they have thaught that it depends on mass , formula says T = C√(h/g) and T is only proportional to height or distance , then how there can be a relation between mass and time, what made them to make a research on this, answer from a researcher in this field will be great.
 
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  • #2
Im a bit rusty but this sounds like you are referring to the possibility that gravitational and inertial mass could be different.

For example we can write...

GMm/r^2 = ma

Where m on the left is the gravitational mass and m on the right is the inertial mass. Normally we assume these are the same so the mass m cancels. That makes the acceleration a independent of m. But what if it's not exactly the same.
 
  • #3
CWatters said:
Im a bit rusty but this sounds like you are referring to the possibility that gravitational and inertial mass could be different.

For example we can write...

GMm/r^2 = ma

Where m on the left is the gravitational mass and m on the right is the inertial mass. Normally we assume these are the same so the mass m cancels. That makes the acceleration a independent of m. But what if it's not exactly the same.
Okk , wohoo you made me think a lot , how can we say that a same particle can have two masses.
 
  • #4
parshyaa said:
scientist are trying to prove that time taken to reach ground when a object is dropped does depends on mass (in small amount)
Why wouldn't it?
An incorrect assumption is that the only one of the masses under mutual gravitational.
Both masses move towards one another.
 
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  • #5
This is guesswork, and it's because the OP didn't ask a good question.

A good question: "In the video at this link, at 4:58, Prof. X says Y. Can you explain how Y and Z can both be true?"
A bad question: "In one of his videos, Prof. X says something that might have been Y. I don't understand/"
 
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  • #6
It is generally expected that inertial and gravitational mass are equivalent. The reason people are looking for a difference is because that would be big news. It's human nature to want to set yourself apart from the crowd. What better way to do that then proving that physics is radically different then everyone thought? So, people keep rechecking old theories with ever greater and greater acuracy, hoping to prove them wrong and find new physics. Sometimes, very rarely, it works, and progress is made. :-)
 
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  • #7
256bits said:
Why wouldn't it?
An incorrect assumption is that the only one of the masses under mutual gravitational.
Both masses move towards one another.
This classical treatment may be all that's involved. The OP doesn't make it clear.
Can the OP give a link to the particular lecture that they are quoting from?
 
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  • #8
, go to this link and you will get walter lewin's first lecture , he discusses all this at the end of video
 
  • #9
parshyaa said:
, go to this link and you will get walter lewin's first lecture , he discusses all this at the end of video
time :36.16 minutes
 
  • #10
Lewin says that people are checking on what we think we know by performing ever more sensitive experiments.
 
  • #11
Vanadium 50 said:
Lewin says that people are checking on what we think we know by performing ever more sensitive experiments.
Why they are checking , formula simply shows that time depends on height only then why do we check for mass
 
  • #12
Because physics is an experimental science, and we want to verify that the formulas we use are correct to the best of our ability.
 
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  • #13
Vanadium 50 said:
Because physics is an experimental science, and we want to verify that the formulas we use are correct to the best of our ability.
Ok how can you say that they are only verifying their formula
 
  • #14
In Newtonian mechanics (two body problem):

The universality of free fall is always true. The time of free fall is affected by the mass of both bodies.

The acceleration of body A is affected only by the mass of body B, and the acceleration of body B is affected only by the mass of body A.

If the mass of free falling body A is changed, it's acceleration will not change, but the time of free fall will change.

If I'm understanding the op post correctly you may find the above statements confusing or even contradictory, but they are all true. I puzzled over this for a long time. It's one of those things where once you get it, it will be an aha moment. Until you understand why the above statements are all true, I think it would be unwise to try and understand the concepts of active, passive, and inertial mass.
 
  • #15
parshyaa said:
Ok how can you say that they are only verifying their formula

I could repeat what I said, only louder, but I don't think it would help.
 
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  • #16
parshyaa said:
Ok how can you say that they are only verifying their formula
What are you trying to say? You seem to be suggesting 'something' is wrong but you are not specifying just what is wrong.
 
  • #17
In General Relativity, a force is felt when a body accelerates in spacetime, suggesting inertial and gravitational mass might be two ways of looking at the same thing.
 
  • #18
parshyaa said:
Why they are checking , formula simply shows that time depends on height only then why do we check for mass
The formula that you are referring to has limitations. It is usually used for measurements near the Earth surface where the value of h is limited. g is not necessarily a constant. It changes with a change in the value of h, thus the limitation. In addition to the value of g being affected by the value of h, it is also affected by the value of the combined masses of both bodies. So to get a more precise value for T we should check for mass also.
 
  • #19
parshyaa said:
Ok how can you say that they are only verifying their formula
Because that's the way that Physics is done. If there is no experimental evidence (and that includes finding that something is NOT a factor) then a theory is not acceptable.
Dimensional Analysis is very powerful at generating ideas and theories but it is not enough because the formula that it's applied to may not actually be correct.
 
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  • #20
A more accurate equation for free fall time can be derived from Kepler's third law:
gif.gif

This equation has the advantage that it accounts for both the distance R and the masses M and m. But it also has the disadvantage that M and m are considered to be point masses. So you would need to account for the physical size of the bodies.
 
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  • #21
TurtleMeister said:
A more accurate equation for free fall time can be derived from Kepler's third law:
gif.gif

This equation has the advantage that it accounts for both the distance R and the masses M and m. But it also has the disadvantage that M and m are considered to be point masses. So you would need to account for the physical size of the bodies.
That is a unique rendering of Kepler's Law for free fall I've not seen. However, if I'm not mistaken Kepler eqn. for period of circular orbital motion should be equivalent to the oscillation period of m through a frictionless hole in the center of large Mass, M, if it has uniform mass density. In that case the free fall period would place m at center of mass, M in 1/4th the period, making the numerical constant merely pi/2 in your above eqn. Where does the extra factor of sq.rt. 2 come from?
 
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  • #22
There seems to be an obvious mistake in what he says.

He says:
Time (is proportional to) height^a x Applemass^b x Earthmass^cAnd then he claims the dimensional analysis proves this must be wrong. But any math would say that PROPORTIONAL means EQUAL WITH A CONSTANT.

So:
Time (is proportional to) Y

means:
Time = kY

And k may have any units. We do not require Planck's constant to be dimensionless (it isn't). Or the Ideal Gas constant to be dimensionless (it isn't). So when he takes a proportionality, and does dimensional analysis, he is not being careful. All he really can conclude is that the dimensions of the constant must cancel everything except the time unit.

I apologize if I've missed an important point, but I skipped to the point in the lecture where the problem is discussed.
 
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  • #23
Afaiaa, Kepler's laws were not to do with free fall and didn't involve Mass, at all but with the geometry and timing of planetary motion. They were arrived at in order to explain observed data and they did not involve any Physics as such. Newton was the one to do that. https://www.mtholyoke.edu/courses/mdyar/ast223/orbits/orb_lect.html
Kepler's law refers to 'swept areas' and, for Simple harmonic oscillation through a hole in the Earth, the swept area is zero.
I really can't see where all this is going. Is there any doubt about the Classical Physics involved here? Lewin's wording was a bit loose and I think he was just being mischievous and showing the risks of relying on Dimensional Analysis. He wanted to make his students think a bit harder and not just to take notes and learn them off by heart.
The thread is causing a number of people to worry about the validity of fundamental stuff and that is a shame.
 
  • #24
sophiecentaur said:
Afaiaa, Kepler's laws were not to do with free fall and didn't involve Mass, at all but with the geometry and timing of planetary motion. They were arrived at in order to explain observed data and they did not involve any Physics as such. Newton was the one to do that. https://www.mtholyoke.edu/courses/mdyar/ast223/orbits/orb_lect.html
Kepler's law refers to 'swept areas' and, for Simple harmonic oscillation through a hole in the Earth, the swept area is zero.
I really can't see where all this is going. Is there any doubt about the Classical Physics involved here? Lewin's wording was a bit loose and I think he was just being mischievous and showing the risks of relying on Dimensional Analysis. He wanted to make his students think a bit harder and not just to take notes and learn them off by heart.
The thread is causing a number of people to worry about the validity of fundamental stuff and that is a shame.
Sorry for this thread ,but he said that time of free fall does depends on mass , if any budy proved this then he will get a nobel prize and scientists are buisy to crack this. Suppose they have proved that yes it does depends on mass , then what will happen to the formula for time t, what is wrong in arguing that inertial mass and gravitational mass can be different[then this argument will raise a question how can a object have two mass] , oh god I am confused and making others too
 
  • #25
parshyaa said:
,but he said that time of free fall does depends on mass

He said no such thing.
 
  • #26
Yah he didn't said that , but he said that scientist are working on this field(it means scientists may thinks that time does/does not depends on mass). I just want to know what made them to do a research on it , you said that it is for varification of physics formula, then can you give me a link where it is written that experimental verification showed that time of free fall does or does not depends on mass.
 
  • #27
parshyaa said:
if any budy proved this then he will get a nobel prize
I will tell my buddies then.
 
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  • #28
parshyaa said:
he said that time of free fall does depends on mass
Vanadium 50 said:
He said no such thing.
parshyaa said:
Yah he didn't said that

There is no point in discussing anything whatever with someone who will write things he knows not to be true.
 
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  • #29
Pet Scan said:
That is a unique rendering of Kepler's Law for free fall I've not seen. However, if I'm not mistaken Kepler eqn. for period of circular orbital motion should be equivalent to the oscillation period of m through a frictionless hole in the center of large Mass, M, if it has uniform mass density. In that case the free fall period would place m at center of mass, M in 1/4th the period, making the numerical constant merely pi/2 in your above eqn. Where does the extra factor of sq.rt. 2 come from?
Here's the Wikipedia page for that equation:
https://en.wikipedia.org/wiki/Free-fall_time
 
  • #30
TurtleMeister said:
Here's the Wikipedia page for that equation:
https://en.wikipedia.org/wiki/Free-fall_time
Thank you TurtleM for the derivation...
The usual (standard) Kepler eqn. that I was trying to reconstruct by squaring your equation is; T^2 / R^3 = 4(pi)^2 / G(M+m) ... but apparently the factor 1/32 kept appearing..
I think this clears it up here:(from your article)...
"Note that T (orbit) in the above equation, is the time for the mass to fall in a highly eccentric orbit, make a "hairpin" turn at the central mass at nearly zero radius distance, and then returns to R when it repeats the very sharp turn. This orbit corresponds to nearly linear motion back and from distance R to distance 0. As noted above, this orbit has only half as long a semimajor axis (R/2) as a circular orbit with radius R (where the semimajor axis is R), and thus the period for the shorter high-eccentricity "orbit" is that for one with an axis of R/2 and a total orbital pathlength of only twice the infall distance. Thus, by Kepler's third law, with half the semimajor axis radius it thus takes only (1/2)3/2 = (1/8)1/2 as long a time period, as the "corresponding" circular orbit that has a constant radius the same as the maximal radius of the eccentric orbit (which goes to essentially zero radius from the primary at its other extreme).

The time to traverse half the distance R, which is the infall time from R along an eccentric orbit, is the Kepler time for a circular orbit of R/2 (not R), which is (1/32)1/2 times the period P of the circular orbit at R. For example, the time for an object in the orbit of the Earth around the Sun, to fall into the Sun if it were suddenly stopped in orbit, would be P / (sq.rt.32) where P is one year..."

Since the first equation (Point masses) is somewhat useless, I included the free fall oscillating in a hole of a Large Mass and concluded it would be equivalent to Kepler's Orbital eqn. for uniform mass density...
They derived a similar result (there is an equivalent equation as the pt. mass eqn.) for extended mass of uniform mass distribution... if M >> m.

Quite interesting...thanks for the link.
Pet Scan
 
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  • #31
parshyaa said:
Sorry for this thread ,but he said that time of free fall does depends on mass , if any budy proved this then he will get a nobel prize and scientists are buisy to crack this. Suppose they have proved that yes it does depends on mass , then what will happen to the formula for time t, what is wrong in arguing that inertial mass and gravitational mass can be different[then this argument will raise a question how can a object have two mass] , oh god I am confused and making others too

@parshyaa (and Sophiecentaur) and whoever else...Maybe I can clarify a bit...Hopefully. It seems that the confusion is arising because there seems to be some confusion about which mass, (central mass or orbiting mass) you guys are referring to when commenting (it needs to be clarified) AND also because someone (Turtlemeister) used a "free -fall" equation based upon Kepler's 3rd law of ORBITAL motion...(which, BTW, is mass dependent) .. Let me explain>..and maybe it will help...maybe..LOL...It will require you to look at the equation briefly. OK, don't stop reading yet, this will be simple, not like my previous post.

Kepler's Law states (as mentioned by sophiecentaur) that an orbital planet sweeps out equal areas in equal times. What this means is that the orbital period, T, squared divided by the orbital Radius (or semi-major axis) CUBED is equal to a CONSTANT for ALL planets revolving around the CENTRAL MASS. Yes, amazingly the ratio of the orbital period squared to the orbital radius cubed is THE SAME value for ANY planet or asteroid or anything orbiting the sun.... Now what Sopie didn't mention is that this CONSTANT is equal to 4 (pi)^2 / GM...where M is the large Mass of the central body...(and G is the "gravitational constant".) This "Kepler" constant is dependent only on the central mass, say the sun for example, as long as the orbiting planets (or whatever) have "negligible" mass compared to the sun. As soon as a planet's mass becomes appreciable, then its mass, m, must be included in the calculation.

This Kepler orbital equation of motion can be manipulated to arrive at free-fall motion, (to which Turtlemeister alluded)...but this is not typical... This no doubt caused some confusion...

The amazing genius of Kepler's equation is that it is applicable for all bodies orbiting around the same central mass. For example,,,ALL satellites orbiting Earth must follow the same Kepler equation (except now using mass of Earth as big M) . IOW, all satellites with the same orbital radius must have the same orbital period...(and even satellites in elliptical orbits have the same orbital period provided we substitute its semi-major axis for radius, R.) This is because the formula depends only upon the mass of Earth and the satellites have "negligible" mass compared to that of earth.
Pres. Eisenhower in 1957, being greatly troubled, for example, when Russia sent the first orbiting satellite (Sputnik) over America, asked US scientists," How can we determine how big (how massive) this Russian satellite is?" The response was , "We can't ... even if we know its orbital period and orbital radius".
Why ? Because the mass of the orbiting satellite does not enter into the equation of motion...only that of the central mass, (earth) ...providing that the satellite isn't a big bugger like that on the movie "Independence Day" ! (LOL).

NOW, having said all that, the above stuff really says almost nothing about "gravitational" verses "inertial" mass. To really enter into that discussion you must start with NEWTON's equations...which deal with INERTIAL mass via F= ma...and combine it with gravitational Force equations like F= GMm / R^2... which gives the force between two masses.
I think I've said enough for now. Clear as mud, right?
Pet Scan
 
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  • #32
During free fall : ma = GMm'/r^2 , I think Newtons gravitational formula is formed for rest masses of a object (I am not shure )
When object falls down, its velocity increases , therefore according to this formula[ m = m'/√ {1-(v^2/c^2)}] , as velocity increases mass of a object also increases (by a tiny amount) , therefore m in LHS is different from m' of RHS therefore a = GMm'/mr^2 , ∴ accelaration depends on mass and it tells that time also depends on mass(for a very very very very small fraction but it does depends on mass) , this is just my thinking , so somebudy please tell me what is wrong in this .
 
  • #33
Classical: Using Kepler's Law, which is the result of and inverse square law relationship is a bit dodgy, imo, when describing the behaviour of a 'through the Earth' pendulum, which involves a very different bit of Physics which gives a SHM.
I know that the resulting period is the same but, without some further detailed proof about the equivalence of the two processes (neither of which were discussed by Kepler, of course) it doesn't get us very far.
GR: In any case, the thread continues to hover between Classical and GR and Lewin's presentation is based on Classical and his Dimensional Analysis assumes things about the relationship that don't follow into GR. For a start, his time and distance variables will be changing in a GR way that he is not including in his lecture. This is all proving nothing.
 
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  • #34
I just now had a chance to take a look at the section of Walter Lewin's lecture that the op is questioning. I think that the "very fancy experiments by very prestigious physicist" that he refers to are actually tests of the equivalence principle. And to be more precise, I think he is referring to tests of the equivalence principle as it relates to inertial and gravitational mass. Even though many of these tests have been performed by simply dropping objects from a height, this can only work when M>>m, such as M=Earth and m=any ordinary object. If you had an instrument sensitive enough (doesn't exist with current technology), or your test mass was massive enough, you could indeed detect a change in free fall time when the mass of the falling object is changed. You can see that in the equation that I posted.

Here's what the equivalence principle says:

Einstein's statement of the equality of inertial and gravitational mass:
A little reflection will show that the law of the equality of the inertial and gravitational mass is equivalent to the assertion that the acceleration imparted to a body by a gravitational field is independent of the nature of the body.

Notice that it says the acceleration imparted to a body by a gravitational field is independent of the nature of the body. So, if we were to change the mass of free falling body m, then it should have no effect on the acceleration of free falling body m. And that is true. However, changing the mass of free falling body m would have an effect on the acceleration of body M. And that would cause a change in the free fall time.

Keep in mind that the accelerations mentioned above are relative to the center of mass of the two bodies, NOT the relative acceleration. This is sometimes a source of misunderstandings in this type of discussion.
 
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  • #35
Handy test objects could be Planets? Any discrepancy between the two masses would / could be revealed in the details of their orbits, perhaps.
 

1. How does the mass of an object affect its time of free fall?

The time of free fall is directly proportional to the mass of an object. This means that the greater the mass of an object, the longer it will take to fall to the ground.

2. Is the time of free fall the same for all objects regardless of their mass?

No, the time of free fall is not the same for all objects. It depends on the mass of the object, as well as other factors such as air resistance and gravitational force.

3. Why does the time of free fall depend on mass?

This is because of the force of gravity. Objects with a greater mass have a greater gravitational force acting on them, which causes them to accelerate at a faster rate and take longer to reach the ground.

4. Does the shape of an object affect its time of free fall?

The shape of an object does not have a significant impact on its time of free fall. As long as the mass and other factors are the same, objects of different shapes will have the same time of free fall.

5. How is the time of free fall calculated for objects with different masses?

The time of free fall can be calculated using the formula t = √(2h/g), where t is the time, h is the height, and g is the acceleration due to gravity. This formula takes into account the mass of the object, as well as other factors such as air resistance and gravitational force.

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