Lorentz force between two moving charges

In summary: In the case of the magnetic field, the momentum of the field itself is what carries the momentum around (just like the ball carries the momentum of the thrower).
  • #1
Universeer
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Two charges are moving mutually perpendicular to each other in space with constant velocities.

The moment one charge crosses over the line of path of second charge the force on 1st charge (located just behind the 2nd charge moving away from it) appear to be zero (Magnetic field due to 2nd charge along its line of path is zero) while force on second charge due to 1st is non zero!
That violates Newton's 3rd law.

What am i missing here?
 
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  • #2
It might be easier to see what is going on if you work in a frame in which one of the particles is at rest. Compare with the frame in which the other is at rest.
 
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  • #3
Universeer said:
Summary: Lorentz force between moving Charges, violates Newton's 3rd law.

Two charges are moving mutually perpendicular to each other in space with constant velocities.

The moment one charge crosses over the line of path of second charge the force on 1st charge (located just behind the 2nd charge moving away from it) appear to be zero (Magnetic field due to 2nd charge along its line of path is zero) while force on second charge due to 1st is non zero!
That violates Newton's 3rd law.

What am i missing here?
1) You have to look at the total EM-force, not just the magnetic component.

2) Newton's 3rd law in the sense of instantaneous forces in fact doesn't always apply for EM-interactions. But it does apply in the more general sense of momentum conservation, if you account for the momentum in the EM-field.
 
  • #4
A.T. said:
2) Newton's 3rd law in the sense of instantaneous forces in fact doesn't always apply for EM-interactions. But it does apply in the more general sense of momentum conservation, if you account for the momentum in the EM-field.

Can you Give an example?
I'll look for total EM force part

Thanks.
 
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  • #5
Universeer said:
Can you Give an example?
Two wires, one carrying a current and one not. Turn on the current in the "off" wire. It immediately feels a force from the magnetic field of the other wire, but it takes finite time for the magnetic field from the new current to reach the other wire. If you don't account for the momentum carried by the field you get a short period where one wire is accelerating and the other isn't.

It's analogous to me throwing a ball to you. If you forget about the momentum of the ball then my reaction to throwing the ball and your reaction to catching it both apparently violate momentum conservation. But that's because you forgot about the momentum of the "force carrier".
 
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1. What is the Lorentz force?

The Lorentz force is the force experienced by a charged particle in an electric and magnetic field. It is the combination of the electric force, caused by the electric field, and the magnetic force, caused by the magnetic field.

2. How is the Lorentz force calculated?

The Lorentz force is calculated using the equation F = q(E + v x B), where F is the force, q is the charge of the particle, E is the electric field, v is the velocity of the particle, and B is the magnetic field.

3. What is the direction of the Lorentz force?

The direction of the Lorentz force is perpendicular to both the electric and magnetic fields and is determined by the right-hand rule. If the particle has a positive charge, the force will be in the direction of the thumb when the fingers of the right hand point in the direction of the velocity.

4. How does the Lorentz force affect the motion of charged particles?

The Lorentz force can change the direction and speed of charged particles. If the force is perpendicular to the velocity, it will cause the particle to move in a circular path. If the force is parallel to the velocity, it will cause the particle to accelerate in the same direction as the force.

5. What are some real-world applications of the Lorentz force?

The Lorentz force is responsible for many phenomena in our daily lives, such as the operation of electric motors, the deflection of charged particles in particle accelerators, and the behavior of charged particles in Earth's magnetic field. It is also used in various technologies, including magnetic levitation trains and magnetic resonance imaging (MRI) machines.

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