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This is a derivation of Larmor's formula which describes the power contained in electromagnetic radiation. The steps followed are the ones from Walter Lewin's 8.03 class at MIT.
On the way to the formula, I derive the expression for the Poynting vector of electromagnetic radiation. The dependence on "sine squared" comes out in the wash. The Poynting vector expression shows that no power is radiated immediately ahead or immediately behind the charged particle; furthermore, it shows that the maximum power is radiated transversely.
This is an important result that is used in the study of antennas.