L can also be solved for in terms of the current angle, , !, R and RL, and also in terms
of VS, VR , !, R and RL. The derivation of these expressions are left as exercises at the end
of the chapter.
L can also be solved for in terms of the current angle, , !, R and RL, and also in termsof VS, VR , !, R and RL. The derivation of these expressions are left as exercises at the endof the chapter.
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