I've been meditating on a question for a week or more and not seeing how to resolve it. It concerns conservation of momentum with electromagnetic forces.positive.
Consider a wire carrying a current and a stationary charge a small distance from it. Let's assume the current is carried by negative charges moving is a static matrix of positive charges, as is usually the case. The stationary charge for now is
If the current is increasing with time, the magnetic vector potential at the stationary charge will likewise be increasing, and pointing in the same direction as the current (i.e. opposite to the actual electron motion). Because the vector potentialis increasing, there will be an electric field directed in the opposite direction. As a result the positive charge will accelerate in the same direction as the electrons.
The acceleration of the electrons will induce a "radiation resistance", which will appear as a force on the accelerating electrons that will resist the acceleration. In other words, the force required to accelerate the electrons will be slightlygreater than that required to accelerate their mass. This force is a rate of change of momentum. This extra momentum has to go somewhere, but it isn't going into the electrons.
Conservation of momentum requires that this extra momentum be accounted for. The obvious answer is that the extra momentum is transferred to the stationary charge (and other charges much further away). This works, because the stationary charge willbe accelerated in the same direction as the electrons are being accelerated, provided the stationary charge is positive.
But what about if the stationary charge is negative? In that case the charge will accelerate in the opposite direction, and its momentum will be in the opposite direction. The electrons in the wire will feel the same radiation resistance, however, sohow is momentum conserved?
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