Inverse square law and Kepler's third law

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Discussion Overview

The discussion centers on the relationship between the inverse square law and Kepler's third law, exploring how these concepts are derived and their implications in both gravitation and electrostatics. Participants examine historical context, mathematical deductions, and experimental foundations related to these laws.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Historical
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that the inverse square law for gravitation was deduced from Kepler's third law, while others argue it is the opposite, with Newton's law of gravitation leading to Kepler's laws.
  • One participant describes how Coulomb's law was derived from experimental measurements of forces between charged objects, suggesting it was not deduced in the same way as gravitational laws.
  • A participant presents a mathematical deduction connecting centripetal force and Kepler's law, proposing that this leads to an inverse square relationship, but seeks validation of this approach.
  • Another participant mentions that a more rigorous proof of the inverse square law would involve considerations of polar orbits and the constancy of angular momentum.
  • Some participants note that Kepler's laws were based on empirical observations rather than mathematical proofs until Newton's development of calculus.
  • There is a discussion about the relative accuracy of electrostatic forces compared to gravitational forces, with references to experimental deviations from the inverse square law.
  • Several participants provide historical context about Kepler and Tycho Brahe's contributions to astronomy and the development of these laws.

Areas of Agreement / Disagreement

Participants express differing views on the historical relationship between Kepler's laws and the inverse square law, with no consensus reached on the correct deduction process for Coulomb's law. The discussion remains unresolved regarding the implications of these laws in both gravitational and electrostatic contexts.

Contextual Notes

Some arguments rely on specific assumptions about the nature of gravitational and electrostatic forces, and the discussion includes references to the limitations of Kepler's laws as approximate rather than exact. The mathematical deductions presented are contingent on the validity of the assumptions made by participants.

Reshma
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The inverse square law for gravitation was deduced from Kepler's third law.
So how was the inverse square law for electrostatics(Coulomb's law) deduced?
 
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The inverse square law for gravitation was deduced from Kepler's third law.
WRONG, it is the other way around...
So how was the inverse square law for electrostatics(Coulomb's law) deduced?
Does it matter?
Gauss' Law if you like...
 
vincentchan said:
WRONG, it is the other way around...

GET THIS:
Kepler (1571-1601) worked out empirical laws governing planetary motions.
Tycho Brahe (1546-1601) compiled extensive data from which Kepler was able to derive the three laws of planetary motion that now bear his name.

Newton(1642-1727) showed that his law of gravitation LEADS to Kepler's laws.

Does it matter? Gauss' Law if you like...
Explain it
 
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Coulomb experimentally measured the forces exerted on charged objects with a variety of charges and distances between them, and came up with the force law.
 
Here is the deduction according to me:

Centripetal force is given by:

F_c = m\omega^2r

Angular velocity is: \omega = \frac{2\pi}{T}

Hence acceleration is :
a_c = \omega^2r = r(\frac{2\pi}{T})^2 = \frac{4\pi^2r}{T^2}

By Kepler's Law: T^2 \propto r^3

Replacing the denominator:

a_c\propto \frac{r}{r^3} \propto \frac{1}{r^2}

This acceleration is same as gravitational acceleration a_g. Since forces varies as acceleration: \vec F\propto a_g

\vec F\propto\frac{1}{r^2}

P.S.--->Someone please let me know if this is right.

Thank you.
 
What is the analogy for electrostatics?
 
Interestingly Kepler was Tyco Brahe's assistant. Tyco Brahe's extensive calculations led Kepler to the laws that we now know as Kepler's Laws of Planetary Motion.

You might be interested in seeing this: http://www.glenbrook.k12.il.us/gbssci/phys/Class/circles/u6l3b.html

Also (please correct me if I'm wrong), Newton began the notion of calculus and used it to prove the two Shell Theorems that we use so frequently in electrostatics and gravitation without bothering much about them. He also discovered that with the sun at one focus, the force required to keep planets in an elliptical orbit was purely radial and varied as the inverse square of this radius. This obvious looking proposition has a very interesting and mathematically englightening proof (in fact many) in older "terse" texts on mechanics.

In other words you can start out with a general force function (without assuming anything) and derive that it must be inverse square for the kind of motion that there is (on paper of course--because in reality there is some deviation).

Finally you might be interested to know that (source = Krane), extensive laboratory experiments reveal that the deviation of electrostatic forces from inverse square dependence is far less than that of graviational forces. In othe words, if you write either force function as proportional to r^{-(2+ \delta)} then \delta = 10^{-4} for gravitational forces and \delta = 10^{-16} for electrostatic forces...which suggests that electrostatic forces are truer inverse square forces than are gravitational forces.

I apologize for some of the content in this post is not germane to the present discussion, but I thought I'd throw it in nevertheless.

Cheers
vivek
 
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Reshma said:
Here is the deduction according to me:

Centripetal force is given by:

F_c = m\omega^2r

Angular velocity is: \omega = \frac{2\pi}{T}

Hence acceleration is :
a_c = \omega^2r = r(\frac{2\pi}{T})^2 = \frac{4\pi^2r}{T^2}

By Kepler's Law: T^2 \propto r^3

Replacing the denominator:

a_c\propto \frac{r}{r^3} \propto \frac{1}{r^2}

This acceleration is same as gravitational acceleration a_g. Since forces varies as acceleration: \vec F\propto a_g

\vec F\propto\frac{1}{r^2}

P.S.--->Someone please let me know if this is right.

Thank you.

While it is conceptually not wrong to show the connection between Kepler's Law and inverse square fields as you have done, this normally isn't the way it is proved (see for example, Central Orbits in Dynamics treatise). Kepler's Law holds only approximately by the way.

A more rigorous proof would involve considerations of polar orbits and deriving an equation of orbit and then showing that the angular momentum constancy, zero tangential force (or equivalently purely radial force), center of force = focus, orbit = elliptical lead to the inverse square field. For circular orbits however, your proof is acceptable iff you can show separately that Kepler's Third Law holds in the form you have used.

Cheers
vivek
 
Interestingly Kepler was Tyco Brahe's assistant. Tyco Brahe's extensive calculations led Kepler to the laws that we now know as Kepler's Laws of Planetary Motion.

Kepler was actually concerned with the specific problem of planetary motion in the gravitational field of the sun. A more precise statement of his third law would therefore be: the square of the periods of the various planets are directly proportional to the cube of their major axes.

Also (please correct me if I'm wrong), Newton began the notion of calculus and used it to prove the two Shell Theorems that we use so frequently in electrostatics and gravitation without bothering much about them. He also discovered that with the sun at one focus, the force required to keep planets in an elliptical orbit was purely radial and varied as the inverse square of this radius. This obvious looking proposition has a very interesting and mathematically englightening proof (in fact many) in older "terse" texts on mechanics.

Yes Newton had discovered the gravitation law but delayed its publication till he found a substantial proof to support them which are of the shell theorems.

In other words you can start out with a general force function (without assuming anything) and derive that it must be inverse square for the kind of motion that there is (on paper of course--because in reality there is some deviation).

Well, from the information I've gathered, Kepler's laws were largely based on rigorous observations rather than mathematical proof till Newton invented Calculus. Same with electrostatics.

Finally you might be interested to know that (source = Krane), extensive laboratory experiments reveal that the deviation of electrostatic forces from inverse square dependence is far less than that of graviational forces. In othe words, if you write either force function as proportional to r^{-(2+ \delta)} then \delta = 10^{-4} for gravitational forces and \delta = 10^{-16} for electrostatic forces...which suggests that electrostatic forces are truer inverse square forces than are gravitational forces.

The deviation can also be largely due to the fact that gravitational forces operate over extremely large distances unlike the electrostatic force.
 
  • #11
Reshma said:
GET THIS:
Kepler (1571-1601) worked out empirical laws governing planetary motions.
Tycho Brahe (1546-1601) compiled extensive data from which Kepler was able to derive the three laws of planetary motion that now bear his name.

Newton(1642-1727) showed that his law of gravitation LEADS to Kepler's laws.


Explain it


What does that represent...?

Daniel.
 
  • #12
dextercioby said:
What does that represent...?
that's mean Kepler died at age of 30...
 
  • #13
Nope,Kepler died much older.And besides,the 3-rd law was disovered ~1616...:wink:

Daniel.
 
  • #14
Reshma said:
The inverse square law for gravitation was deduced from Kepler's third law.
So how was the inverse square law for electrostatics(Coulomb's law) deduced?

Coulomb's law is based on experiment. It was not deduced. Just like Newton's force law, P=mf.

It is true that Johannes Keplar and Tycho Brahe's research preeceded Newton's discovery of the inverse sqare law,but Newton 'historically' arrived at the inverse square law independently.
It was then it was found to be aligned with "Keplar's Laws".
 
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  • #15
And that is Johannes Kepler...(sic).And that "foce law" is F=dp/dt...

Daniel.
 
  • #16
Why precisely gravitational field isn't as true an inverse square field as the electric field cannot be purely because of large distances of operation. The electric field is closer to ideality so to say. Firstly we cannot precisely determine why the gravitational field is nonideal and say that THAT is the truth. In principle, we could attribute it to several things (in classical physics minus relativity one could attribute it to the nonideal shapes of sources that set up the fields...if you consider only the Earth then the field isn't perfectly inverse square--there are deviations because of its oblate spheroidal shape and the like).

So I wouldn't attribute it to one thing alone.
 
  • #17
Reshma said:
Well, from the information I've gathered, Kepler's laws were largely based on rigorous observations rather than mathematical proof till Newton invented Calculus. Same with electrostatics.

You would probably know that Kepler's third law isn't completely accurate? If you tend to think otherwise you might want to read AS Ramsey or Kleppner.
 
  • #18
What do you mean it is not completely accurate...?Sure,for a 2 body system (isolated,no perturabations to trajectories) it should take into account the movement around the common center of mass (usually that is achieved by putting the reduced mass in the equations)...

What's new...?

Daniel.
 
  • #19
maverick280857 said:
You would probably know that Kepler's third law isn't completely accurate? If you tend to think otherwise you might want to read AS Ramsey or Kleppner.
Kepler's third laws would be completely accurate if there was only one planet. Newton's Universal Law of Gravitation flows directly from Kepler's third law.

AM
 
  • #20
Andrew,two-body-system interracting through Newton's gravity force...:wink:

Daniel.
 
  • #21
Reshma said:
Kepler (1571-1601) worked out empirical laws governing planetary motions.
dextercioby said:
What does that represent...?

vincentchan said:
that's mean Kepler died at age of 30...

I apologise to Dextercioby and Vincentchan for the typo.
The correct year is: 1571-1630
 
  • #22
maverick280857 said:
Why precisely gravitational field isn't as true an inverse square field as the electric field cannot be purely because of large distances of operation. The electric field is closer to ideality so to say. Firstly we cannot precisely determine why the gravitational field is nonideal and say that THAT is the truth. In principle, we could attribute it to several things (in classical physics minus relativity one could attribute it to the nonideal shapes of sources that set up the fields...if you consider only the Earth then the field isn't perfectly inverse square--there are deviations because of its oblate spheroidal shape and the like).

So I wouldn't attribute it to one thing alone.

I did not say that is the only reason. It could possibly be one of the reasons.
 
  • #23
Andrew Mason said:
Kepler's third laws would be completely accurate if there was only one planet. Newton's Universal Law of Gravitation flows directly from Kepler's third law.

AM

YES, I've deduced it in this post! :wink:
 
  • #24
maverick280857 said:
You would probably know that Kepler's third law isn't completely accurate? If you tend to think otherwise you might want to read AS Ramsey or Kleppner.

Hi Vivek, thanks for all the replies!

I have "Introduction to Newtonian Attraction" by AS Ramsey. Can you please point out that particular chapter(because I did not find much references made to Kepler's laws in this book)?

I hate to say this, but after prolonging this discussion this far I haven't received a single clear-cut answer
 
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  • #25
Also note, Kepler's third law is rigorously true for the electron orbits in the Bohr atom (Source: Classical Mechanics: Herbert Goldstein).
 
  • #26
Reshma said:
Also note, Kepler's third law is rigorously true for the electron orbits in the Bohr atom (Source: Classical Mechanics: Herbert Goldstein).
In the Bohr atom the force on the electon is a central force that varies as 1/r^2. That gives you Kepler's third law. But the Bohr atom is not an accurate model of physical reality.

AM
 
  • #27
Andrew Mason said:
In the Bohr atom the force on the electon is a central force that varies as 1/r^2. That gives you Kepler's third law. But the Bohr atom is not an accurate model of physical reality.

AM

Ah finally someone hits the nail on the head. You see its like this: you start out with an assumed model of the motion. Then you use some other "laws" or "ideas" to show that something (which you're trying to show) holds 'rigourously'. But the assumption need not be correct in real life as Andrew has so rightly pointed out. As for reality, there are perturbations in orbits due to several reasons. In a crude way perhaps it is right to say that a perturbation term (which cannot be correctly described in our world) gets added to the differential equation of every point motion referred to an inertial or noninertial frame. For all practical purposes in undergraduate studies, this term equals zero.

Now, regarding the book reference, to be honest I haven't even heard of this book by AS Ramsey. I was referring to Mechanics by AS Ramsey parts I and II (sections on Central Orbits/Polar Orbits).

Cheers
vivek
 

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