a zero-voltage-switching, physically flexible multilevel

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A Zero-Voltage-Switching, Physically Flexible Multilevel GaN DC-DC Converter Derek Chou, Yutian Lei, and Robert Pilawa-Podgurski University of Illinois at Urbana-Champaign Presented by: Derek Chou

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Page 1: A Zero-Voltage-Switching, Physically Flexible Multilevel

A Zero-Voltage-Switching, Physically Flexible Multilevel GaN DC-DC Converter

Derek Chou, Yutian Lei, and Robert Pilawa-Podgurski

University of Illinois at Urbana-ChampaignPresented by: Derek Chou

Page 2: A Zero-Voltage-Switching, Physically Flexible Multilevel

Outline

Motivation Hardware Design Zero-Voltage Switching Experimental Results Future Work

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Page 3: A Zero-Voltage-Switching, Physically Flexible Multilevel

Motivation – Lightweight, flexible power converter

Wind turbine tip de-icing Deliver high power de-icing capabilities

while conforming to aerodynamic constraints

Electric machine exterior Deliver high power in a small and

conformal package 3D cooling structures Aerospace applications Resistant to thermal cycling Lightweight, high specific and

volumetric power density Research goals High power density High efficiency, electrical & thermal Lightweight

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Source: http://www.plainswindeis.anl.gov/

Source: Pilawa Group

Page 4: A Zero-Voltage-Switching, Physically Flexible Multilevel

Goal

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High power density power converter

Flexible PCB substrate

Images: Pilawa Research Group (left) http://www.directindustry.com/industrial-manufacturer/printed-circuit-board-flexible-90300.html (right)

Page 5: A Zero-Voltage-Switching, Physically Flexible Multilevel

Goal

5

High power density power converter

Flexible PCB substrate

Images: Pilawa Research Group (left, bottom) http://www.directindustry.com/industrial-manufacturer/printed-circuit-board-flexible-90300.html (right)

Lightweight, flexible high power density power converter

Page 6: A Zero-Voltage-Switching, Physically Flexible Multilevel

Flexible PCBs

Polyimide substrate – flexible, high-voltage resistantMultiple copper layers possible Conform to 3D structures Thermal cycling resistant Soldered components not restricted by rigid substrate Need small passive components to leverage flexibility

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Page 7: A Zero-Voltage-Switching, Physically Flexible Multilevel

7-level FCML design Phase-shifted PWM

signals Natural capacitor

balancing Lower switch stress Smaller passive

components

Hardware Design – Flying Capacitor Multilevel Converter

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Page 8: A Zero-Voltage-Switching, Physically Flexible Multilevel

Vsw = Vin – VC3 + VC1= Vin – 3Vin/6 + Vin/6 = 4Vin/6

Vsw = Vin – VC5 + VC3= Vin – 5Vin/6 + 3Vin/6 = 4Vin/6

finductor = (N – 1) * fswitch

Hardware Design – Flying Capacitor Multilevel Converter

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Vin 5Vin / 6 4Vin / 6 3Vin / 6 2Vin / 6 Vin / 6

Page 9: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

Turn on switches when VDS = 0 V Benefits Large reduction of switching losses Further reduce passive component size Very low switch stress

Challenges Higher-frequency switching Larger inductor ripple Full ZVS operation is dependent on load

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Page 10: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

Turn on switches when VDS = 0 V Benefits Large reduction of switching losses Further reduce passive component size Very low switch stress

Challenges Higher-frequency switching Larger inductor ripple Full ZVS operation is dependent on load

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Page 11: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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t = ti1 to t = ti2

Both switches off (td,f); CS1B discharges through the inductor

Page 12: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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t = ti2

S1B turns on (ZVS)

Page 13: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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t = ti2 to t = ti3

(other switch pairs commutate)

Page 14: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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t = ti2 to t = ti3

(other switch pairs commutate)

Page 15: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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t = ti2 to t = ti3

(other switch pairs commutate) Inductor current is negative when t = ti3

Page 16: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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t = ti3

S1B turns off (ZVS), inductor current is negative

Page 17: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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t = ti3 to t = ti4

Both switches off (td,r); CS1B charges through the inductor

Page 18: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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t = ti4

S1A turns on (ZVS), inductor current is still negative

Page 19: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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t = ti4 to t = T Inductor current ramps up to positive value Cycle repeats after t = T

Page 20: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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Arbitrary switch pairs behave similarly ZVS achieved on all switch pairs

Page 21: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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Arbitrary switch pairs behave similarly ZVS achieved on all switch pairs

Page 22: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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Arbitrary switch pairs behave similarly ZVS achieved on all switch pairs

Page 23: A Zero-Voltage-Switching, Physically Flexible Multilevel

Zero-Voltage Switching

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Arbitrary switch pairs behave similarly ZVS achieved on all switch pairs

Page 24: A Zero-Voltage-Switching, Physically Flexible Multilevel

Hardware – Flexible PCB

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Side View

Page 25: A Zero-Voltage-Switching, Physically Flexible Multilevel

ZVS Control

Automatic ZVS control, as a function of output load Switching frequency controls ZVS operation Duty cycle controls output voltage

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Δippiout

Page 26: A Zero-Voltage-Switching, Physically Flexible Multilevel

ZVS Implementation

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Inductor current ripple maximized at certain duty ratios For a fixed switching frequency and input voltage, overall

current ripple decreases as number of levels, N, increases

Page 27: A Zero-Voltage-Switching, Physically Flexible Multilevel

Experimental Results – FCML ZVS

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Switching frequency 200-500 kHz at each switch Ripple frequency 1.2-3.0 MHz at the inductor D = 0.58, D = 0.25 Inductor ripple current maximized

Current Ripple Characteristics for 7-level FCML

Page 28: A Zero-Voltage-Switching, Physically Flexible Multilevel

Experimental Results

Automatic ZVS control, D = 0.58 vs D = 0.25

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Vin = 200 V, Vout = 116 V, D = 0.58 or D = 0.25, fsw = 200-500 kHz

Page 29: A Zero-Voltage-Switching, Physically Flexible Multilevel

Experimental Results

Variable frequency – high efficiency over wide load range Fixed frequency only achieves ZVS in a narrow range

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Vin = 200 V, Vout = 116 V, D = 0.58, fsw = 200-500 kHz

Page 30: A Zero-Voltage-Switching, Physically Flexible Multilevel

Experimental Results

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Parameter Notes Value

Output Power Tested 250 W

Switching Frequency Per Switch 200–500 kHz

Effective Frequency At Inductor 1.2–3.0 MHz

Weight Excl. controller 17.5 g

Volumetric Power Density Bounded by prism 109 W/in3 (6.65 W/cm3)

Volumetric Power Density Excl. empty space 902 W/in3 (6.65 W/cm3)

Specific Power Density Excl. controller 14 kW/kg

Page 31: A Zero-Voltage-Switching, Physically Flexible Multilevel

Conclusions

ZVS possible for FCML converters Thermal management of high power density

converters Flexible PCB allows for mechanical compliance and

routing of electrical signals in the 3D space 3D electro-mechanical integration for heatsinking Further layout development for optimization of FCML

operations

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Page 32: A Zero-Voltage-Switching, Physically Flexible Multilevel

Choice of Passive Components

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70 mJ of capacitor energy storage

70 mJ of inductor energy storage

Page 33: A Zero-Voltage-Switching, Physically Flexible Multilevel

Experimental Results – Loss Distribution

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Pout = 150 W, D = 0.58 ZVS – heat concentrated in inductor Hard switching – heat concentrated in switches

ZVS Hard switching