Violation of Newtons Third law

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SUMMARY

The discussion centers on the apparent violation of Newton's Third Law in electromagnetism, particularly in the context of charged particles and their interactions. Participants clarify that while it seems violated, this is due to the omission of the momentum of electric and magnetic fields. When this momentum is included, Newton's Third Law holds true, reaffirming the conservation of momentum and angular momentum. The conversation also touches on the limitations of Newton's laws in the framework of special relativity, where the exchange of momentum between fields and particles complicates the application of the Third Law.

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  • Understanding of Newton's Laws of Motion
  • Familiarity with electromagnetic theory
  • Knowledge of conservation laws in physics
  • Basic principles of special relativity
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  • Study the role of electromagnetic fields in momentum conservation
  • Explore advanced topics in electromagnetism, such as field momentum
  • Investigate the implications of special relativity on classical mechanics
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Physics students, educators, and anyone interested in the foundational principles of mechanics and electromagnetism, particularly those exploring the intersections of classical and modern physics.

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TheBlackNinja said:
I've heard many times that Newtons third law is violated in electromagnetism, but I never knew why.
I found this link http://www.google.com/url?sa=t&sour...dkMvK2nhw&sig2=jwk3H90wOMVq8cPtcPk7UQ&cad=rja
saying that actually it is not violated.

Is it correct? Is it violated somewhere else?
It is violated, either that or F=ma is violated.

From the link:
link provided by OP said:
If we sum the magnetic forces of two charged particles on each other, we find this apparent violation of Newton’s third law (after some manipula- tion): [equation elided]

The reason for the apparent violation is that the momentum of the electric and magnetic fields has been omitted. When that momentum is included (an advanced topic), Newton’s third law is again obeyed.
I beg to differ. What is true is that when that momentum is included (an advanced topic), the conservation laws are again obeyed.

One way to look at Newton's third law is that it is a special case of the more generic laws of conservation of momentum and angular momentum. The circumstances under which Newton's third law derives from the conservation laws are when forces are central in nature and depend on position only, and when the field that mediates the force does not itself store momentum or angular momentum. Various electromagnetic forces fail on all three accounts, so why would you expect Newton's third law to hold in such a case?
 
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If this is true then why don't we have reactionless drives?
 
TurtleMeister said:
If this is true then why don't we have reactionless drives?
Because momentum and angular momentum are conserved quantities.
 
Probably too advanced for me, so I'll just take your word for it. I've always thought of the third law and the conservation of momentum to be simply two different ways of viewing the same thing. Violate one then you violate the other.
 
TurtleMeister said:
Probably too advanced for me, so I'll just take your word for it. I've always thought of the third law and the conservation of momentum to be simply two different ways of viewing the same thing. Violate one then you violate the other.

Newton's third law is true for Newton's gravity - the sun attracts the Earth and the Earth attracts the sun at the same time - even though both are far from each other. How can each know how hard the other is pulling immediately? In Newtonian physics, there is no upper limit to the speed of things, so there's no problem there. But this is obviously doesn't fit in with special relativity - so Newton's third law doesn't hold in special relativity.

In special relativity, the local exchange of momentum is between fields and particles. A particle feels a force due to a field. But there isn't a simple way to say that a field feels a force due to a particle. So to keep the spirit of Newton's third law for fields and particles, we ascribe momentum to both, and say that momentum is conserved.
 
Oh, I see. Thanks for the simple explanation.
 

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