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8. AC POWER CIRCUITS by Ulaby & Maharbiz
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Overview
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Linear Circuits at ac Instantaneous power Average power Power at any instant of timeAverage of instantaneous power over one period Power delivery (utilities) Electronics (laptops, mobile phones, etc.) Logic circuits Power is critical for many reasons: Note: Power is not a linear function, cannot apply superposition
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Instantaneous Power for Sinusoids Power depends on phases of voltage and current Trig. Identity: Constant in time (dc term) ac at 2
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Average Value Sine wave Truncated sawtooth
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Average Value for These properties hold true for any values of φ 1 and φ 2
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Effective or RMS Value Equivalent Value That Delivers Same Average Power to Resistor as in dc case For current given by Effective value is the (square) Root of the Mean of the Square of the periodic signal, or RMS value Hence: Similarly,
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Average Power Note dependence on phase difference
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Average Power Sinceand a similar relationship applies to I, Power factor angle: 0 for a resistor = 90 degrees for inductor ‒ 90 degrees for capacitor
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ac Power Capacitors Capacitors (ideal) dissipate zero average power = 0
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ac Power Inductors Inductors (ideal) dissipate zero average power = 0
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Complex Power Phasor form defining “real” and “reactive” power
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Power Factor for Complex Load Inductive/capacitive loads will require more from the power supply than the average power being consumed Power supply needs to supply S in order to deliver P av to load Power factor relates S to P av
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Power Factor
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Power Factor Compensation Introduces reactive elements to increase Power Factor
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Example 8-6: pf Compensation
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Maximum Power Transfer Max power is delivered to load if load is equal to Thévenin equivalent Max power transfer when Set derivatives equal to zero
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Example 8-7: Maximum Power Cont.
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Example 8-7: Maximum Power
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Three Phase
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Y & Delta
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Y-Source Connected to a Y-Load
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Multisim Measurement of Power
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Multisim Measurement of Complex Power Complex Power S
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Summary
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