Questions about Big G: Constant of Proportionality

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In summary, Big G is a constant of proportionality in the universal law of gravitation. It is required to line up the terms in the equation F = (Gm1m2)/r^2. This is different from F = ma, where the units of force were chosen to correspond with the equation. G is not a representation of a proportionality between active and passive masses, it is simply a necessary component in the equation.
  • #1
TurtleMeister
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According to Wikipedia, Big G is a constant of proportionality. When speaking of proportionality one thinks of two quantities which can vary in such a way as to have a constant ratio of something. If that is true, then in the case of Big G, what are the quantities, and what is the something?
 
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  • #2
TurtleMeister said:
According to Wikipedia, Big G is a constant of proportionality. When speaking of proportionality one thinks of two quantities which can vary in such a way as to have a constant ratio of something. If that is true, then in the case of Big G, what are the quantities, and what is the something?
So you have already read this:
http://en.wikipedia.org/wiki/Gravitational_constant
including
7cdf733b81cd2b83d434160241d6023c.png

and
981c4a7801639525969c8d798aca28ce.png

and you ask what is proportional to what, and what the units of G are?
 
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  • #3
Thank you for the reply A.T. I think I'm understanding the proportionality better now. However, I am still confused about something. In Newton's second law of motion there is no constant of proportionality (F = ma). Here there is a direct relationship between force, mass, and acceleration. But in the universal law of gravitation, the proportionality G is required. Why is that? I understand the inverse square of the distance. But why does it appear that the mass used in the universal law of gravitation is different from the mass used in the second law of motion?
 
  • #4
I believe the reason for the lack of constant of proportionality in F=ma is due to how force is defined. For example, having a definition of mass and acceleration, we define the force of 1N to be that which is produces a 1m/s^2 acceleration of a 1kg body. Now, we COULD have defined force differently, perhaps using the universal law. In this case, we would say something like 1N is the force two 1kg bodies exert on each other at a distance of 1m. I think then you would actually get the constant of proportionality, G, in f=ma somewhere.

Cheers.
 
  • #5
For gravity, "G" is inside "a". To line up the terms, F = (m)(a) corresponds to F = (m1) (G m2/r^2). The last thing in parentheses is the acceleration of m1.
 
  • #6
Nabeshin said:
I believe the reason for the lack of constant of proportionality in F=ma is due to how force is defined. For example, having a definition of mass and acceleration, we define the force of 1N to be that which is produces a 1m/s^2 acceleration of a 1kg body. Now, we COULD have defined force differently, perhaps using the universal law. In this case, we would say something like 1N is the force two 1kg bodies exert on each other at a distance of 1m. I think then you would actually get the constant of proportionality, G, in f=ma somewhere.
Are you saying that 1N in the universal law of gravitation has (or could have) a different definition than 1N in the second law of motion? I must be misunderstanding you because that doesn't make any sense.
mikelepore said:
For gravity, "G" is inside "a". To line up the terms, F = (m)(a) corresponds to F = (m1) (G m2/r^2). The last thing in parentheses is the acceleration of m1.
Yes, I understand that G is used for a force due to gravity. I guess I should rephrase the question.

Disregarding the inverse square of the distance - I understand that, why is a constant of proportionality required for a force on an object due to gravity and not for a force on the same object due to acceleration (such as that produced by a rocket)?
 
  • #7
TurtleMeister said:
Are you saying that 1N in the universal law of gravitation has (or could have) a different definition than 1N in the second law of motion? I must be misunderstanding you because that doesn't make any sense.

That is indeed what I'm saying, but note that the choice of the symbol N is a bit deceiving, since we think of 1 Newton = 1 kg*m/s^2. This would be a different unit, but corresponding to our concept of force. In particular, it would have dimensions mass^2/length^2.
 
  • #8
TurtleMeister said:
why is a constant of proportionality required for a force on an object due to gravity and not for a force on the same object due to acceleration (such as that produced by a rocket)?
That is just an artifact of the used unit system. You can use a unit system where G = 1, so it doesn't appear in the formula:
http://en.wikipedia.org/wiki/Geometrized_unit_system
 
  • #9
That is interesting A.T. But I'm not sure it clears things up for me. For example, just like G, pi is a constant of proportionality. If we change the unit system in an equation so that pi does not appear then we have not erased what it represents, we have only hidden it. The proportionality is still there. Also, if we change the unit system for universal gravitation then wouldn't we also have to change it for the second law of motion thereby putting us right back where we started from with the discrepancy?
 
  • #10
Thank you A.T., Nabeshin, and mikelepore for the responses.

I'm still unclear about what BigG is a proportionality of. All the text I have read does not go into detail. It appears to have the units of force, but force of what? The two masses?

I know that there are three types of mass, or properties of mass. Active, passive, and inertial. I know that the m in F = ma is inertial. But I'm not sure about F = (GMm) / r2. I'm thinking active and passive. That would explain the discrepancy between universal gravitation and the second law of motion. But what about G? Does it represent the proportionality between the active and passive mass? Wouldn't a proportionality between the masses violate the equivalence principle?
 
  • #11
Forget about the equivalence principle, active/passive masses, and the like. GMm/r^2 is part of Newtonian equation, so general relativity is irrelevant.

There were no units of force at the time of Newton. The SI unit of force, the Newton, was chosen so that F=ma. It could have been chosen so that F=Mm/r^2; then F=kma because the force needed to accelerate 1 kg at 1 m/s^2 isn't the same as the force between 2 1-kg objects separated by 1 m.
 
  • #12
TurtleMeister said:
I'm still unclear about what BigG is a proportionality of. All the text I have read does not go into detail. It appears to have the units of force, but force of what? The two masses?

G is the constant of proportionality between force (which has units of Newtons as defined by F = ma) and Mm/r^2 (which has units of kg^2/m^2). Accordingly, G has units of N*m^2/kg^2 in order to make the units balance on both sides of F = GMm/r^2.

In principle, we could define the gravitational force between two 1-kg masses separated by 1 m to be a new unit of force, and call it, say, the "Cavendish" (Cav). In Cavendish units, the law of gravitation would read simply F = Mm/r^2. The second law of motion would read F = Cma, where C is a proportionality constant with units of Cav/(kg*m/sec^2) = Cav*sec^2/(kg*m).
 
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  • #13
Thanks very much for the replies. I think you guys are saying the same thing as A.T. Sorry, I guess I'm not being very clear on what I'm asking. I understand that the equations can be manipulated by changing the unit system. However, doing so does not change the fact that there is a proportionality difference between the second law of motion and the universal law of gravitation. And that is what my question is about. For example:

a = 3
b = 4
C = 0.25 'constant of proportionality

ab = 12
Cab = 3

C tells me that something in the second equation (either a or b) is 1/4 what it is in the first equation. So in the universal law of gravitation, what is G telling me?
 
  • #14
TurtleMeister said:
For example:

a = 3
b = 4
C = 0.25 'constant of proportionality

ab = 12
Cab = 3
It seems you don't understand what a http://en.wikipedia.org/wiki/Constant_of_proportionality" [Broken] is. In this example C is not a constant of proportionality between two variables.

TurtleMeister said:
C tells me that something in the second equation (either a or b) is 1/4 what it is in the first equation.
They could also be both 1/2 of the first, or any other combination that gives 1/4 as product. So C tells you little here.
 
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  • #15
A.T. said:
It seems you don't understand what a constant of proportionality is. In this example C is not a constant of proportionality between two variables.
I thought it was probably something I was not understanding. Could you possibly give me an example (similar to mine) where C is a constant of proportionality?
 
  • #16
  • #17
F = G mM/r²
ma = G mM/r²
a = G M/r²
a r²/M = G

Is that what you want?
 
  • #18
Ok, I think I understand now. G is the constant of proportionality between the force and the mass? Can I assume that G is so small because of the very weak gravitational force of the mass? And the reason it's not needed for the second law of motion is that the second law of motion does not rely on a gravitational field?
 
  • #19
TurtleMeister said:
Can I assume that G is so small because of the very weak gravitational force of the mass?
G is small because of our choice of units. The only fundamental constants whose values have any physical significance are the dimensionless ones like the fine structure constant. All others are purely an artifact of the chosen system of units.
 
  • #20
So we could change our system of units so that G was large in relation to M? If so, what would happen to F = ma?
 
  • #21
TurtleMeister said:
So we could change our system of units so that G was large in relation to M?
Yes, although IMO it doesn't make sense to "compare apples and oranges" like that.
TurtleMeister said:
If so, what would happen to F = ma?
Nothing.
 
  • #22
I'll give that some thought. It's starting to look like G is not so magical after all. :)

I would to thank everyone who has responded in this thread. You've been very helpful to me. I may return later if I have more questions.

Turtle
 
  • #23
A couple of simpler examples:

1 inch = 0.0254 m
0.0254 = inch * m^-1

0.0254 is the constant of proportionality which relates inches to meters. It's dimensionless because inches and meters have the same dimension, length. The energy of a photon is Planck's constant times the frequency:

E = h*f
h = E*f^-1

Energy is measured in joules, frequency in cycles per second. Planck's constant is 6.626 * 10^-34 J*s. It consists of a number and the appropriate units to relate energy to frequency. Energy and frequency aren't measured in the same units as each other, which is why Planck's constant needs the right units to balance the equation.

Likewise with the gravitational constant G:

m*a = G*M*m*r^-2
G = a * M^-1 * r^2

And G = 6.674 * 10^-11 m^3 * s^-2 * kg^-1. It's the constant of proportionality between force and M*m*r^-2. If we used some system of units other than SI units, these constants might have different values. Coulomb's constant plays the corresponding role for electrical force: m*a = k*Q*q*r^-2, where k stands for Coulombs constant, Q is the charge of what is exerting the force, and q the charge of what is affected by the force.

What do you mean by "the discrepancy between universal gravitation and the second law of motion"?
 
  • #24
Rasalhague said:
What do you mean by "the discrepancy between universal gravitation and the second law of motion"?
Just a poor choice of words. It looked like a discrepancy because of my misunderstanding. Thanks for the examples.
 
  • #25
Ok, I've become confused again and I need your help. In the manual for the Pasco torsion balance there is a procedure for measuring the gravitational constant. The equation used is:

G = (tr2) / (2dm1m2)

which is derived from the law of universal gravitation, with t being the torque on the torsion ribbon, and d being the length of the pendulum bob arm.

G = (Fr2) / (m1m2)

It would appear from these equations that G actually represents a proportionality between the objects mass and the force of it's gravitational field. For example, increasing r2 will cause F to decrease by the same amount (inverse square law). Increasing the mass of m1 and/or m2 will cause the same increase in F. So G always stays the same (constant ratio).

I've never seen G described as a constant of proportionality between an objects inertial mass and it's gravitational mass. If this is correct then why is it not described that way. Or, what am I doing wrong?
 
  • #26
TurtleMeister said:
I've never seen G described as a constant of proportionality between an objects inertial mass and it's gravitational mass. If this is correct then why is it not described that way. Or, what am I doing wrong?
It is not correct. An object's inertial mass is equal to its gravitational mass. Also, G is not dimensionless whereas the ratio of the inertial mass to the gravitational mass is dimensionless (and equal to 1).
 
  • #27
Also, r is not a constant. So any change in r will change the ratio of mass to force. I guess I was up too late last night. Thanks for the reply.
 
  • #28
Yous are all getting confused.
There is a difference between G and g.
g changes and is the force per kilogram due to gravity.
G is a constant (meaning it never changes)

And i could be wrong on this point, but i think it was kepler that first calculated it t^2/r^3 in his third law of planetary motion, where r is the distance between an object and the sun and t is its period.
 
  • #29
Actually there was no confusion between Big G and Little g. The confusion was caused by me being an idiot when it comes to math. :) But I appreciate the input anyway.
 

1. What is the value of the Big G constant?

The value of the Big G constant, also known as the gravitational constant, is approximately 6.674 x 10^-11 cubic meters per kilogram per second squared (m^3/kg/s^2).

2. How was the Big G constant first measured?

The Big G constant was first measured by Henry Cavendish in 1798 using a torsion balance experiment. He measured the force of attraction between two lead spheres and calculated the value of the constant based on the distance between the spheres and their masses.

3. Why is the Big G constant important?

The Big G constant is important because it is a fundamental constant in physics that helps us understand the force of gravity between objects. It is used in many equations, including Newton's law of universal gravitation, and is essential for studying celestial bodies and the behavior of objects in space.

4. Is the Big G constant truly constant?

Yes, the Big G constant is considered to be a universal constant, meaning it does not change over time or in different locations. However, there have been some controversial studies that suggest the constant may vary slightly in different conditions, but these findings have not been widely accepted.

5. Are there any ongoing research or experiments related to the Big G constant?

Yes, there are ongoing efforts to improve the accuracy of the Big G constant measurement and to understand its role in the laws of physics. Some experiments are also exploring the possibility of a varying Big G constant or looking for alternative theories to explain the force of gravity.

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