Slide 1: Circuits with Resistance and Inductance - Power in Inductive Circuits

  • In a circuit containing both resistance and inductance, power is dissipated in both components.
  • Inductive circuits have power factors less than 1 due to phase difference between current and voltage.
  • Power in inductive circuits can be determined using the formulas:
    • Instantaneous power: p(t)=vip(t) = vi
    • Average power: Pavg=1T0Tp(t)dtP_{avg} = \frac{1}{T} \int_{0}^{T} p(t) dt
    • RMS power: Prms=1T0Tp2(t)dtP_{rms} = \sqrt{\frac{1}{T} \int_{0}^{T} p^2(t) dt}
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Slide 1: Circuits with Resistance and Inductance - Power in Inductive Circuits In a circuit containing both resistance and inductance, power is dissipated in both components. Inductive circuits have power factors less than 1 due to phase difference between current and voltage. Power in inductive circuits can be determined using the formulas: Instantaneous power: $p(t) = vi$ Average power: $P_{avg} = \frac{1}{T} \int_{0}^{T} p(t) dt$ RMS power: $P_{rms} = \sqrt{\frac{1}{T} \int_{0}^{T} p^2(t) dt}$