Inverse square law and Kepler's third law

In summary, Kepler's third law of planetary motion is deduced from Tycho Brahe's extensive data. The inverse square law for electrostatics was derived from Coulomb's law. It does not matter which law was first discovered.
  • #1
Reshma
749
6
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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  • #2
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...
 
  • #3
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 :grumpy:
 
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  • #4
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.
 
  • #5
Here is the deduction according to me:

Centripetal force is given by:

[tex]F_c = m\omega^2r[/tex]

Angular velocity is: [tex]\omega = \frac{2\pi}{T}[/tex]

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

By Kepler's Law: [tex]T^2 \propto r^3[/tex]

Replacing the denominator:

[tex]a_c\propto \frac{r}{r^3} \propto \frac{1}{r^2}[/tex]

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

[tex]\vec F\propto\frac{1}{r^2}[/tex]

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

Thank you.
 
  • #6
What is the analogy for electrostatics?
 
  • #7
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 [Broken]

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 [itex]r^{-(2+ \delta)}[/itex] then [itex]\delta = 10^{-4}[/itex] for gravitational forces and [itex]\delta = 10^{-16}[/itex] 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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  • #8
Reshma said:
Here is the deduction according to me:

Centripetal force is given by:

[tex]F_c = m\omega^2r[/tex]

Angular velocity is: [tex]\omega = \frac{2\pi}{T}[/tex]

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

By Kepler's Law: [tex]T^2 \propto r^3[/tex]

Replacing the denominator:

[tex]a_c\propto \frac{r}{r^3} \propto \frac{1}{r^2}[/tex]

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

[tex]\vec F\propto\frac{1}{r^2}[/tex]

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
 
  • #9
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 [itex]r^{-(2+ \delta)}[/itex] then [itex]\delta = 10^{-4}[/itex] for gravitational forces and [itex]\delta = 10^{-16}[/itex] 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 :grumpy:


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 :grumpy:
 
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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
 

1. What is the inverse square law?

The inverse square law is a physical principle that states that the intensity of a physical quantity, such as light or force, is inversely proportional to the square of the distance from the source.

2. How does the inverse square law apply to light?

In the context of light, the inverse square law means that the intensity or brightness of light decreases as the distance from the light source increases. This is because the same amount of light is spread over a larger area, resulting in a lower intensity.

3. What is Kepler's third law?

Kepler's third law, also known as the harmonic law, states that the square of the orbital period of a planet is directly proportional to the cube of the semi-major axis of its orbit. This law relates the motion of a planet around the sun to its distance from the sun.

4. How is Kepler's third law related to the inverse square law?

Kepler's third law and the inverse square law are both based on the same principle of inverse proportionality. Kepler's third law describes the relationship between a planet's orbital period and its distance from the sun, while the inverse square law describes the relationship between the intensity of a physical quantity and the distance from its source.

5. What real-world applications does the inverse square law have?

The inverse square law has many applications in physics and engineering. It is used to calculate the intensity of light from a source, the strength of gravitational or electric fields, and the radiation exposure from a radioactive source. It is also an important concept in understanding the behavior of sound and other waves.

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