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If we consider moving charges alone interacting via Coulomb magnetic forces, Newton's third law does not hold and momentum is not conserved.
Similarly, examples are known in which the law of conservation of angular momentum seems in case of charges in time varying fields.

This happens because the energy angular momentum of the e.m. fields is not taken into account. This page explains
how to derive a conservation law for charges interacting with e.m. fields

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  1. Derivation of angular momentum conservation for charges in electromagnetic fields
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  3. Conservation laws in relativity cannot be simply a statement \( \frac{dQ}{dt}=0\). 

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