Questions about understanding circular motion & the forces involved

[A.T.]

Fictitious forces can be directly measured in the non-inertial frame.

Forces in general cannot be directly observed. We observe effects like acceleration or deformation, and postulate forces to match them. Assuming Newton's gravitation, you need to postulate inertial forces in the free falling frame, to make the net force match the observed acceleration.

 

[A.T.]

In the non-inertial frame, there is no acceleration.

Nonsense. The reference extends to infinity, and isn't limited to a small area with only free falling masses. There are plenty of accelerating objects in that frame.

 

[nrqed]

It is the measurement of gravity in the non-inertial frame that is the problem. Gravity is measured by the acceleration it provides to a unit mass. In the non-inertial frame, there is no acceleration.

AM

But if you look out of a window of the ISS and you see the Earth moving around you, surely the Earth is accelerating as observed in that frame. The non inertial frame of the ISS does not stop at its outer hull.

 

[nrqed]

And I disagree with that view. Fictitious forces can be directly measured in the non-inertial frame. The posited "anti-gravity" fictitious force cannot.

AM

The distinction that you are making seems to be that in the case of gravitational free fall the fictitious force is produced by an intellectual argument, whereas in the other cases it can actually be measured.

AM.

I don't see the problem with using an intellectual argument. We know that all masses produce an attractive gravitational force. We see a planet very nearby. We therefore know that there is a non negligible attractive pull toward the planet. But we are free floating and feel no acceleration. Therefore a (fictitious) force must cancel the gravitational pull.

You seem to say that it is only when we can use a plumb line or a spring scale to measure a force that it must be taken into account. What about the e/m experiment? You have an electron floating in an electric field. The net force is zero, you cannot use a spring scale to measure the gravitational force on the electron, nor the electric force . You use an intellectual argument to argue that the electric force cancel the force of gravity to determine the e/m ratio. That is not controversial!

 

[Andrew Mason]

Newton's universal law of gravitation can be deduced from within an accelerated reference frame. The result is a net inertial force of the form:
F=Km+\frac{GMm}{r^2}

Ok. So you are falling toward an object - a body of unknown mass. How do you determine M? And how do you determine the distribution of mass within the body? The only way to determine that is by measuring your acceleration. But in the non-inertial frame you are in, there is no acceleration.

Though why you would chose to use a non-inertial frame which results in freely falling objects being unaccelerated in only one place is a mystery.

? The free-falling body is always unaccelerated in its non-inertial frame of reference (ie. a frame of reference the body - a frame in which the origin is undergoing non-inertial motion) regardless of the acceleration or rate of change of acceleration that an inertial observer measures. (We are assuming that tidal forces within the body are negligible).

AM

 

[jbriggs444]

Ok. So you are falling toward an object - a body of unknown mass. How do you determine M? And how do you determine the distribution of mass within the body. The only way to determine that is by measuring your acceleration. But in the non-inertial frame you are in, there is no acceleration.

Newton did it. Why can't you?

The free-falling body is always unaccelerated in its non-inertial frame of reference (ie. a frame of reference in which the origin is undergoing non-inertial motion) regardless of the acceleration or rate of change of acceleration that an inertial observer measures. (We are assuming that tidal forces within the body are negligible).

NO NO NO. We are NOT assuming that tidal forces are negligible. We are NOT confined to a small local region. Your post #26 makes no such restriction.

Edit: Are you, perhaps, under the mistaken impression that frames of reference are physical and restrict the set of observations we can make?

 

[A.T.]

The free-falling body is always unaccelerated in its non-inertial frame of reference

But other bodies are accelerated in that frame, and you have to introduce inertial forces to reconcile those accelerations with Newtons 2nd Law.

 

[nrqed]

And I disagree with that view. Fictitious forces can be directly measured in the non-inertial frame. The posited "anti-gravity" fictitious force cannot.

AM

Just to be clear: if you were teaching college physics (not GR but Newtonian physics), would you tell your students that in the ISS there is no force of gravity acting and the proof is that people observe themselves to be free floating? So inside a free falling elevator at the surface of the Earth (ignoring friction, Coriolis force, etc), you would say the same thing: for the people inside there is no force of gravity since they are free floating.?That's what you would tell them? But now, if one analyzes the ISS from the point of view of the ground, would you say that there is a force of gravity on it or not? (I am guessing yes). So you would say that the force of gravity on a given object may be present or not depending on the frame of reference we use to analyze the system? Is that what your point of view?

 

[Andrew Mason]

Just to be clear: if you were teaching college physics (not GR but Newtonian physics), would you tell your students that in the ISS there is no force of gravity acting and the proof is that people observe themselves to be free floating? So inside a free falling elevator at the surface of the Earth (ignoring friction, Coriolis force, etc), you would say the same thing: for the people inside there is no force of gravity since they are free floating.?

I expect the student would have an understanding of Newton's law of motion and gravity from high school so I don't think you are going to get away with telling them that gravity disappears 100 miles above the earth. But it is precisely because there are no inertial pseudo forces required to make Newton's laws of motion work in a free-falling frame of reference that the principle of equivalence was postulated. It is based on Newtonian physics.

If you introduce tidal forces, of course, it is another matter. Then you have to introduce some pseudo force causing the tensions or you go to GR for the better explanation. The fundamental difference between gravity and all other forces is the fact that the force of gravity is proportional to inertial mass (as far was we can tell). As such, inertial forces are not required to treat a free-falling frame (locally) as an inertial frame. I guess I will just leave it at that.

AM

 

[Andrew Mason]

JSo you would say that the force of gravity on a given object may be present or not depending on the frame of reference we use to analyze the system? Is that what your point of view?

Why would you ask such a question?

Would you ask: does the car stop accelerating because the person inside is trying to apply Newton's laws as if he were an inertial observer?

It is not a matter of whether the non-interial observer has the means of figuring out that is frame of reference is accelerating. He assumes it is not and invents fictitious inertial forces to make Newton's laws work as if his non-inertial frame were inertial.

Before wasting your time with these kinds of questions, I suggest you re-read the entire thread and, in particular, my posts 6, 10, 13, 15, 18 and 22 where I think I have made it clear what I have to say on the subject. My purpose was not to provide a treatise on pseudo forces but to simply point out an important difference between gravity and other forces for the OP. I think we can all agree that there is an important difference.

AM

 

[nrqed]

Why would you ask such a question?

Because I am trying to understand your point of view. And I asked several questions before the one you are referring to. But you did not answer any of them and then you ask me why I would ask such a question. So I guess you prefer not to answer any of them and therefore there is no way to continue the discussion.

 

[jbriggs444]

I expect the student would have an understanding of Newton's law of motion and gravity from high school so I don't think you are going to get away with telling them that gravity disappears 100 miles above the earth. But it is precisely because there are no inertial pseudo forces required to make Newton's laws of motion work in a free-falling frame of reference that the principle of equivalence was postulated. It is based on Newtonian physics.

This amounts to a claim that free-falling reference frames are inertial (an eminently reasonable claim). But post #26 claims that they are non-inertial. You cannot have it both ways. Which is it?

 

[Andrew Mason]

This amounts to a claim that free-falling reference frames are inertial (an eminently reasonable claim).

It is not inertial if you apply Newtonian physics. But for purposes of applying Newton's laws of motion, it is locally equivalent to an inertial frame.

But post #26 claims that they are non-inertial. You cannot have it both ways. Which is it?

Why can it not be a non-inertial frame (as analysed Newtonian physics) that is locally indistinguishable from an inertial reference frame (as analysed in Newtonian physics)?

AM

 

[jbriggs444]

Why can it not be a non-inertial frame (as analysed Newtonian physics) that is locally indistinguishable from an inertial reference frame (as analysed in Newtonian physics)?

It can be. But you need to pick one and not keep jumping back and forth, willy nilly without notice as has been your habit in this thread.

 

[Andrew Mason]

It can be. But you need to pick one and not keep jumping back and forth, willy nilly without notice as has been your habit in this thread.

I have always been talking about the frame of reference of a body being accelerated only by gravity and the fact that inertial forces are not needed in order to apply Newton's laws. Read my posts 6, 10, 13, 15,18, 22, 31 for example. What other scenario do you think I have been referring to?

In post 4 the OP stated:

• "What I understand is: In the situation of in an accelerating car, if I put a scale between the seat and my back, a non-zero number would pop up. This is analogous to just standing on a scale right? You would have a "gravity" towards the seat. And this perceived gravity is just the normal force accelerating you. So in short, you'll always perceive gravity in the opposite direction of the net force on you?"

My comment in post 6 was to clarify that if the force accelerating you is gravity, you don't feel that push back into the seat.

• "Gravity is different than all other forces. There is no "inertial force effect" when the acceleration is provided by gravity. When an astronaut orbits the Earth he/she feels no centrifugal (outward) effect - no sensation of centrifugal force."

I am at a complete loss as to why you would think my comment would be controversial.

AM

 

[A.T.]

Why can it not be a non-inertial frame (as analysed Newtonian physics) that is locally indistinguishable from an inertial reference frame (as analysed in Newtonian physics)?

The key word here is "local", while Newtonian inertial frames extend to infinity. The observational local indistinguishability can be matched by different models. And if "Newtonian physics" includes the Newtonian interpretation of gravity, then the non-inertial free falling frame involves an inertial force that opposes gravity.