EE 462 L Spring 2014 Implementation of Unipolar

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EE 462 L, Spring 2014 Implementation of Unipolar PWM Modulation for H-Bridge Inverter (pre-fall

EE 462 L, Spring 2014 Implementation of Unipolar PWM Modulation for H-Bridge Inverter (pre-fall 2009 - but discrete components provide a better sense of how this circuit operates) 1

H-Bridge Inverter Basics – Creating AC from DC Switching rules Either A+ or A–

H-Bridge Inverter Basics – Creating AC from DC Switching rules Either A+ or A– is closed, but never at the same time Either B+ or B– is closed, but never at the same time Vdc A+ Va B+ Load A– ! Vb B– Can use identical isolated firing signals for A+, A–, with inverting and noninverting drivers to turn on, turn off simultaneously Same idea for B+, B– The A+, A– firing signal is a scaled version of Va The B+, B– firing signal is a scaled version of Vb The difference in the two firing signals is a scaled version of Vab 2

! Implementation of Unipolar PWM Vcont is the input signal we want to amplify

! Implementation of Unipolar PWM Vcont is the input signal we want to amplify at the output of the inverter. Vcont is usually a sinewave, but it can also be a music signal. Vcont Vtri −Vcont The implementation rules are: Vcont > Vtri , close switch A+, open switch A– , so voltage Va = Vdc Vcont < Vtri , open switch A+, close switch A– , so voltage Va = 0 –Vcont > Vtri , close switch B+, open switch B– , so voltage Vb = Vdc –Vcont < Vtri , open switch B+, close switch B– , so voltage Vb = 0 Vtri is a triangle wave whose frequency is at least 30 times greater than Vcont. Ratio ma = peak of control signal divided by peak of triangle wave 3 Ratio mf = frequency of triangle wave divided by frequency of control signal

! Implementation of Unipolar PWM Modulation for H-Bridge Inverter Vload Progressively wider pulses at

! Implementation of Unipolar PWM Modulation for H-Bridge Inverter Vload Progressively wider pulses at the center Progressively (peak of narrower pulses sinusoid) at the edges Vdc Unipolar Pulse-Width Modulation (PWM) −Vdc 4

The four firing circuits do not have the same ground reference. Thus, the firing

The four firing circuits do not have the same ground reference. Thus, the firing circuits require isolation. ! Vdc (source of power delivered to load) A+ Local ground reference for A+ firing circuit S S S Load A– Local ground reference for A− firing circuit B+ Local ground reference for B+ firing circuit B– S Local ground reference for B− firing circuit 5

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This year’s circuit 7

This year’s circuit 7

Output of the Comparator Chip Comparator Gives V(A+, A–) wrt. Common (0 V) V(A+,

Output of the Comparator Chip Comparator Gives V(A+, A–) wrt. Common (0 V) V(A+, A–) +12 V from DC-DC chip 1. 5 kΩ +12 V 1. 5 kΩ – 12 V 270 kΩ Vtri 8 1 Comp 5 1 kΩ Vcont 4 Vcont < Vtri Since the comparator compares signals that can be either positive or negative, the comparator must be powered by ±V supply Use V(A+, A–) wrt. – 12 V 270 kΩ –Vcont > Vtri +24 V Vcont > Vtri – 12 V from DC-DC chip 0 V Common (0 V) from DC-DC chip Vcont < Vtri 8

Comparator Gives V(B+, B–) wrt. Common (0 V) Output of the Comparator Chip V(B+,

Comparator Gives V(B+, B–) wrt. Common (0 V) Output of the Comparator Chip V(B+, B–) +12 V from DC-DC chip –Vcont > Vtri +12 V 1. 5 kΩ – 12 V 1. 5 kΩ 270 kΩ Vtri 8 1 Comp 5 1 kΩ Vcont 4 Since the comparator compares signals that can be either positive or negative, the comparator must be powered by ±V supply Use V(B+, B–) wrt. – 12 V 270 kΩ –Vcont – Vcont < Vtri – 12 V from DC-DC chip Common (0 V) from DC-DC chip – Vcont > Vtri +24 V 0 V – Vcont < Vtri 9

This year’s circuit 10

This year’s circuit 10

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+4 V 0 V − 4 V 15

+4 V 0 V − 4 V 15

+24 V 0 V 16

+24 V 0 V 16

+24 V 0 V 17

+24 V 0 V 17

+24 V 0 V − 24 V 18

+24 V 0 V − 24 V 18

+24 V 0 V − 24 V Flat toping indicates the onset of overmodulation

+24 V 0 V − 24 V Flat toping indicates the onset of overmodulation +24 V 0 V − 24 V 19

Approaching a square wave +24 V 0 V − 24 V 20

Approaching a square wave +24 V 0 V − 24 V 20

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