Is action and reaction instantanious?

In summary, the conversation discusses the concepts of action and reaction in physics, particularly in relation to Newton's third law and its implications. The participants also touch on topics such as time, perception, and quantum theories. However, there is no clear consensus or understanding reached on these topics.
  • #71
Andrew Mason said:
There is an important difference between gravity and all other forces, in that there is no inertial effect with a gravitational force.

If all forces were "balanced" by an equal and opposite force there would be no "net force" so there would be no acceleration. Inertia is not a force. It is resistance to change in motion. It only appears to be a force (inertial effect) in the frame of reference of the accelerating body (which is not an inertial frame) when an unbalanced force (other than gravity) is applied to the body. It does not appear to be a force in the inertial frame.

AM
there is inertia with gravity. its just that the force (or rather the field) is proportional to the mass.

yes there could be, would be, and is acceleration even though the net forces are zero. that's exactly what I'm saying. if what you say was true then kirchhoffs law would mean that no current could ever flow.
 
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  • #72
imagine a hypothetical massless charged particle. if acted on by an external electric field it would begin to accelerate. us it did so it would create a magnetic field around itself. this changing magnetic field would produce a force upon the particle that would exactly balance the force from the external electric field. I certainly hope you wouldn't say that that force wasnt a real force.

the behavior of this 'self inductance' is almost identical to the behavior of mass. indeed it was once hypothesized that all mass was the result of self inductance.

so the force of gravity acting on one mass due to another must equal the force of gravity acting on the second due to the first. but the sum of all forces, including those due to inertia, acting on a single object must also be zero. both statements are true and complement one another.further, while what has been said about gravity isn't exactly wrong nevertheless there is no reason to see gravity as being any different from other forces. replace mass with change and reverse the direction of the resulting force and you have the electric field. (excluding relativistic effects like time dilation of course.)
 
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  • #73
granpa said:
yes there could be, would be, and is acceleration even though the net forces are zero.
Newton disagrees. If f=0 then a=0 by the second law.
 
  • #74
and the massless changed particle?
 
  • #75
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  • #76
DaleSpam said:
Newton disagrees. If f=0 then a=0 by the second law.

So when two masses are attracted to each other via gravity, there is a net force? Because obviously a =/= 0, but I can't figure out how there can be a net force.
 
  • #77
there is a net force acting on each individual mass but only if you disregard the force due to inertia.
 
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  • #78
granpa said:
there is a net force acting on each individual mass but only if you disregard the force due to inertia.
In physics, force is defined as dp/dt. You will need a new definition of force if you wish to call inertia a force.

Consider a system that experiences no external force. Masses within that system can exert forces on each other and cause momentum of the individual masses to change with time. All Newton's third law says is that the sum of those forces ie. [itex]\sum dp_i/dt[/itex] must be 0. If you add interia as a force, they would not sum to 0.

AM
 
  • #79
Andrew Mason said:
In physics, force is defined as dp/dt. You will need a new definition of force if you wish to call inertia a force.

Consider a system that experiences no external force. Masses within that system can exert forces on each other and cause momentum of the individual masses to change with time. All Newton's third law says is that the sum of those forces ie. [itex]\sum dp_i/dt[/itex] must be 0. If you add interia as a force, they would not sum to 0.

AM
other forces might be defined that way. but that doesn't contradict what i said.

obviously you can always define all the other forces in terms of any single force.

maybe it would be better to think of force as being defined in terms of energy.

they would not sum to zero? they are zero everywhere so why would the sum not be zero over the whole?
 
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  • #80
granpa said:
there is inertia with gravity. its just that the force (or rather the field) is proportional to the mass.
I did not say there was no inertia. I said there is no inertial effect. The orbiting astronaut feels no centrifugal "force".

AM
 
  • #81
granpa said:
and the massless charged particle?
I am not aware of any massless charged particle. Can you give us an example?

AM
 
  • #82
Andrew Mason said:
I did not say there was no inertia. I said there is no inertial effect. The orbiting astronaut feels no centrifugal "force".

AM

people don't 'feel' the force of air pressure either but its there.
 
  • #83
read post 72

notice the third word
 
  • #84
granpa said:
so the force of gravity acting on one mass due to another must equal the force of gravity acting on the second due to the first. but the sum of all forces, including those due to inertia, acting on a single object must also be zero.
Viewed from the non-inertial frame of the accelerating mass, one must introduce fictitious inertial forces to make use of Newton's laws. Is that what you mean by "forces due to inertia"?

Such "forces" are just artifacts of viewing things from a non-inertial frame.
 
  • #85
I can't understand why so many people have difficulty with this. It seems pretty obvious to me. simply think of mass the way you would self inductance.

no relativity has nothing to do with it.
 
  • #86
granpa said:
other forces might be defined that way. but that doesn't contradict what i said.

maybe it would be better to think of force as being defined in terms of energy.
It may be more useful to use energy rather than force in some situations. In nuclear physics that is exactly what is done: we speak of binding energies and collision energies rather than forces.

they would not sum to zero? they are zero everywhere so why would the sum not be zero over the whole?
I don't follow you here. Kinetic energies are always greater than zero. So a system experiencing no external force may still have significant energy. Think of a star that undegoes a supernova.

AM
 
  • #87
Andrew Mason said:
I don't follow you here. Kinetic energies are always greater than zero. So a system experiencing no external force may still have significant energy. Think of a star that undegoes a supernova.

AM

I don't even know how to begin to answer that. Its clear to me that you are making it all much much more complicated than it really is. stop trying so hard and maybe you will get what I'm saying

are you familiar at all with Kirchoffs law?
 
  • #88
granpa said:
people don't 'feel' the force of air pressure either but its there.
This is not equivalent. A person on the surface of the Earth can measure atmospheric pressure by doing a local experiment. An orbiting astronaut cannot detect gravity by doing a local experiment.

AM
 
  • #89
Andrew Mason said:
This is not equivalent. A person on the surface of the Earth can measure atmospheric pressure by doing a local experiment. An orbiting astronaut cannot detect gravity by doing a local experiment.

AM


once again, I don't even know how to begin to answer. I see no relevance and no contradiction to anything I've said. I think you think I'm saying something complicated when all I'm saying is really very simple.
 
  • #90
granpa said:
I don't even know how to begin to answer that. Its clear to me that you are making it all much much more complicated than it really is. stop trying so hard and maybe you will get what I'm saying

are you familiar at all with Kirchoffs law?
I am not sure how you are using it. Kirchoff's law does not have anything to do with inertia or its electrical equivalent.

AM
 
  • #91
Andrew Mason said:
I am not sure how you are using it. Kirchoff's law does not have anything to do with inertia or its electrical equivalent.

AM

Kirchoffs law has nothing to do with inductance??
 
  • #92
granpa said:
f=ma (ma=inertial force)
f=f
action=reaction
f-f=0
OK, first the action=reaction part is simply wrong. Action and reaction refer to Newton's 3rd law and action-reaction pairs act on different bodies. F=ma refers to Newton's 2nd law and acts on the same body. So even if you want to call ma a force it is not a reaction force to f since it is acting on the same body that f is acting on.

Now, the remainder of what you did is mathematically correct and leads to the trivially true assertion 0=0. This algebraic manipulation can be done for any formula.

W = f.d
W = W
0 = 0

x(t) = 1/2 a t² + v0 t + x0
x(t) = x(t)
0 = 0

Yes you can always do it, but in doing so you completely lose the meaning of the original expression.

It looks like you are using the D'Alembert approach which can be useful in certain circumstances, but you need to understand what it is doing. https://www.physicsforums.com/showthread.php?t=219929" is a thread on the subject. It should generally be avoided because of the conceptual confusion it causes, and it should only be applied when the specific problem demands it.

In the end, if you are talking about inertial reference frames then ma is not a force and the body accelerates. If you are talking about the non-inertial rest frame of an accelerating body (as D'Alembert does) then there is a fictitious inertial force (like the Coriolis force) of magnitude ma and the body does not accelerate. This force that exists only in the non-inertial frame does not follow Newton's 3rd law because its source is the non-inertial reference frame and not an interaction with another object.
 
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  • #93
WarPhalange said:
So when two masses are attracted to each other via gravity, there is a net force? Because obviously a =/= 0, but I can't figure out how there can be a net force.
There is a net force on each object (Newtonian gravity). So the Earth pulls the moon "down" and the moon pulls the Earth "up". The force on the moon is equal and opposite to the force on the earth, per Newton's 3rd law.
 
  • #94
Andrew Mason said:
In physics, force is defined as dp/dt. You will need a new definition of force if you wish to call inertia a force.

Consider a system that experiences no external force. Masses within that system can exert forces on each other and cause momentum of the individual masses to change with time. All Newton's third law says is that the sum of those forces ie. [itex]\sum dp_i/dt[/itex] must be 0. If you add interia as a force, they would not sum to 0.
This is correct. Inertia is only a force in non-inertial reference frames where it appears as a so-called ficticious force. In non-inertial reference frames the momentum of an isolated system is not conserved (hence the designation "non-inertial").
 
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  • #95
granpa said:
they would not sum to zero? they are zero everywhere so why would the sum not be zero over the whole?
Because they are not zero everywhere. You can choose a non-inertial frame where anyone object is at rest, but in that reference frame an object which is not experiencing any real forces will still experience the inertial force and will therefore accelerate. The net effect is a violation of the conservation of momentum for an isolated system, or equivalently, a violation of Newton's 3rd law. This is simply what happens in non-inertial frames.

By the way, none of this has anything to do with relativity, this is all just Newtonian mechanics.
 
  • #96
granpa said:
f=ma (ma=inertial force)
f=f
action=reaction
f-f=0

I have no idea what inertia is (and don't wish to find out), so I am not addressing that. But I think some subscripts are missing on the equations.

Consider a two particle system:
m1, v1, a1: mass, velocity and acceleration of particle 1
m2, v2, a2: mass, velocity and acceleration of particle 2
F12: force on particle 1 due to the effect of particle 2
F21: force on particle 2 due to the effect of particle 1

F12=m1a1 [E1: Newton's 2nd law for particle 1]
F21=m2a2 [E2: Newton's 2nd law for particle 2]
F12=-F21 [E3: Newton's 3rd law, action and reaction are equal and opposite]

We can rearraange E3 as you did: F12+F21=0 [E3b]

From E3 or E3b, neither F12 nor F21 is necessarily zero, only equal and opposite. From E1 and E2, assuming m1 and m2 positive and constant, F12 and F21 must be zero only if a1 or a2 are zero.

But we can combine E3b with E1 and E2:
F12+F21=m1a1+m2a2=d(m1v1+m2v2)/dt=0,
which says that there is no net force on both particles considered together (not separately) and that total momentum does not change over time, ie. momentum is conserved.
 
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  • #97
granpa said:
Kirchoffs law has nothing to do with inductance??
You may be thinking of Lenz's law.

AM
 
  • #98
nobody has addressed my very simple question. what about a hypothetical massless charged particle? it has self inductance so it would accelerate under the influence of an external field in exactly the same way that a massive particle would. the force due to self inductance exactly balancing the force due to the external field. net force is zero yet it still accelerates.

thats all I'm saying. I'm comparing the behavior of mass to the behavior of self inductance.

as for defining force/mass, I can imagine a video game like universe in which time distance and velocity are all well defined but possessing nothing that we would recognize as force or mass. so I would guess that both arise simultaneously if the system possesses some kind of symmetry. possibly related to conservation laws and Noethers theorem.

I'm just guessing at this point.
 
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  • #99
granpa said:
nobody has addressed my very simple question. what about a hypothetical massless charged particle? it has self inductance so it would accelerate under the influence of an external field in exactly the same way that a massive particle would.

I think this is not quite what you had in mind, but is it close?
Xiaochao Zheng's notes on "Radiation reaction and electron's self energy -- an unsolved problem" http://www.jlab.org/~xiaochao/teaching/PHYS343/tex/chap11-6.pdf
 
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  • #100
atyy said:
I think this is not quite what you had in mind, but is it close?
Xiaochao Zheng's notes on "Radiation reaction and electron's self energy -- an unsolved problem" http://www.jlab.org/~xiaochao/teaching/PHYS343/tex/chap11-6.pdf


this hypothetical massless charged particle isn't a point change. it has finite diameter. and no I don't know whits holding it together. it doesn't matter. maybe superglue.
 
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  • #101
granpa said:
nobody has addressed my very simple question. what about a hypothetical massless charged particle? it has self inductance so it would accelerate under the influence of an external field in exactly the same way that a massive particle would. the force due to self inductance exactly balancing the force due to the external field. net force is zero yet it still accelerates.
There is, of course, no such thing as a massless charged particle. A massless particle travels at the speed of light relative to all inertial frames, so it cannot accelerate.

A particle with charge q in an electric field [itex]\vec E[/itex] experiences a force [itex]\vec F[/itex] = q[itex]\vec E[/itex]. The only thing that affects its acceleration is its mass. [itex]\vec F[/itex] = q[itex]\vec E[/itex] = ma. There is no other force.

AM
 
  • #102
Andrew Mason said:
There is, of course, no such thing as a massless charged particle. A massless particle travels at the speed of light relative to all inertial frames, so it cannot accelerate.

A particle with charge q in an electric field [itex]\vec E[/itex] experiences a force [itex]\vec F[/itex] = q[itex]\vec E[/itex]. The only thing that affects its acceleration is its mass. [itex]\vec F[/itex] = q[itex]\vec E[/itex] = ma. There is no other force.

AM
whoa. a moving charge has energy in its magnetic field. this energy must be supplied by the external force. it would not move at the speed of light.
 
  • #103
granpa said:
this hypothetical massless charged particle isn't a point change. it has finite diameter. and no I don't know whits holding it together. it doesn't matter. maybe superglue.

Xiaochao Zheng's notes that I linked to above also treated the non-point charge case.

Jammer, Concepts of Mass, Chapter 11
http://books.google.com/books?hl=en...X&oi=book_result&resnum=6&ct=result#PPA136,M1

Acceleration-dependent self-interaction effects as a possible mechanism of inertia
Vesselin Petkov
http://arxiv.org/abs/physics/9909019
 
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  • #104
granpa said:
whoa. a moving charge has energy in its magnetic field. this energy must be supplied by the external force. it would not move at the speed of light.
?? A moving charge has energy in its magnetic field only relative to a charge in a different intertial frame of reference. The magnetic field disappears for a charge in the same intertial frame of reference.

A charged particle cannot move at the speed of light because all particles with charge have mass. Light will always travel at the speed of light, c, relative to a particle with mass.

The only inertia, or resistance to change in speed, of a charged particle in an electric field is due to the mass of the charged particle, as explained in my previous post. (At relativistic speeds, the apparent inertia increases due to relativistic effects).

AM
 
  • #105
atyy said:
Xiaochao Zheng's notes that I linked to above also treated the non-point charge case.

Jammer, Concepts of Mass, Chapter 11
http://books.google.com/books?hl=en...X&oi=book_result&resnum=6&ct=result#PPA136,M1

Acceleration-dependent self-interaction effects as a possible mechanism of inertia
Vesselin Petkov
http://arxiv.org/abs/physics/9909019

Apparently a massless charged particle is not classically possible even if it is not a point charge. All discussions use F=dp/dt, ie. no change in momentum unless there is a net force. granpa: your superglue is referred to by Jackson (Classical Electrodynamics, Wiley 1998) as Poincare stresses.

References that seem to be regarded as standard, but not available for free are:
A.D. Yagjian, Relativistic Dynamics of a Charged Sphere, 2nd ed. Springer 2006
F. Rohrlich, Classical Charged Particles, 3rd ed. (World Scientific 2007)

On arXiv:
Radiation reaction of a classical quasi-rigid extended particle
Rodrigo Medina
http://arxiv.org/abs/physics/0508031
 
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