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ECE 442 Power Electronics1 Series-Resonant Inverter
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ECE 442 Power Electronics2 Operation T 1 fired, resonant pulse of current flows through the load. The current falls to zero at t = t 1m and T 1 is “self – commutated”. T 2 fired, reverse resonant current flows through the load and T 2 is also “self-commutated”. The series resonant circuit must be underdamped, R 2 < (4L/C)
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ECE 442 Power Electronics3 Operation in Mode 1 – Fire T 1
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ECE 442 Power Electronics4
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5 To find the time when the current is maximum, set the first derivative = 0
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ECE 442 Power Electronics6 To find the capacitor voltage, integrate the current The current i 1 becomes = 0 @ t=t 1m
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ECE 442 Power Electronics7
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8 Operation in Mode 2 – T 1, T 2 Both OFF
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ECE 442 Power Electronics9 t 2m
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ECE 442 Power Electronics10 Operation in Mode 3 – Fire T 2
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ECE 442 Power Electronics11
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ECE 442 Power Electronics12
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ECE 442 Power Electronics13
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ECE 442 Power Electronics14 Summary -- Series Resonant Inverter
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ECE 442 Power Electronics15 To avoid a short-circuit across the main dc supply, T 1 must be turned OFF before T 2 is turned ON, resulting in a “dead zone”. This “off-time” must be longer than the turn-off time of the thyristors, t q. The maximum possible output frequency is
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ECE 442 Power Electronics16 Series Resonant Inverter Coupled Inductors
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ECE 442 Power Electronics17 Improvement in performance When T 1 turned ON, voltage @ L 1 is as shown, voltage @ L 2 in same direction, adding to the voltage @ C This turns T 2 OFF before the load current falls to 0.
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ECE 442 Power Electronics18 Half-Bridge Series Resonant Inverter Note: L 1 = L 2 C 1 = C 2
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ECE 442 Power Electronics19 This configuration reduces the high-pulsed current from the dc supply Power drawn from the source during both half-cycles of the output. Half of the current is supplied from the associated capacitor, half of the current is supplied from the source.
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ECE 442 Power Electronics20 Full-Bridge Series-Resonant Inverter
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ECE 442 Power Electronics21 Characteristics of the full-bridge inverter This configuration provides higher output power. Either T 1 -T 2 or T 3 -T 4 are fired. Supply current is continuous but pulsating.
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ECE 442 Power Electronics22 Example 8.1 – Analysis of the Basic Resonant Inverter L 1 = L 2 = L = 50μH C = 6μF R = 2Ω V s = 220V f o = 7kHz t q = 10μs
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ECE 442 Power Electronics23 Determine the resonant frequency The resonant frequency in Hz
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ECE 442 Power Electronics24 Determine the turn-off time t off
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ECE 442 Power Electronics25 Determine the maximum permissible frequency
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ECE 442 Power Electronics26 Determine the peak-to-peak capacitor voltage
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ECE 442 Power Electronics27 Determine the peak load current
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ECE 442 Power Electronics28 Sketch the instantaneous load current, capacitor voltage, and dc supply current
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ECE 442 Power Electronics29 Calculate the rms load current
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ECE 442 Power Electronics30 Using MATHCAD, I o = 44.1Amperes
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ECE 442 Power Electronics31 Determine the output power
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ECE 442 Power Electronics32 Determine the average supply current
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ECE 442 Power Electronics33 Determine the average, peak, and rms thyristor currents
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ECE 442 Power Electronics34 rms Thyristor Current Using MATHCAD
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