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At very high frequencies, the parallel RL circuit behaves as
- AA pure inductive circuit
- BAn LC circuit
- CA pure capacitive circuit
- DA pure resistive circuit
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Inductive reactance is $({X_L} = 2\pi fL)$
At very high frequencies, inductive reactance will be infinity and it acts as an open circuit.
Hence parallel RL circuit at this condition becomes pure resistive circuit.
At very high frequencies, inductive reactance will be infinity and it acts as an open circuit.
Hence parallel RL circuit at this condition becomes pure resistive circuit.