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Soft-Switching in DC-DC Converters:
Principles, Practical Topologies,
Design Techniques, Latest Developments
Raja Ayyanar
Arizona State University
Ned Mohan
University of Minnesota
Eric Persson
International Rectifier
©2002, N. Mohan, R. Ayyanar, E. Persson APEC 2002
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Objectives
•
What is soft-switching?
•
Basic principles
•
Concentration on a few
popular topologies
•
Design techniques
•
Computer simulations
•
New developments
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What is Soft-Switching
•
Switching transitions occur under favorable
conditions – device voltage or current is zero
•
Reduced switching losses, switch stress,
possibly low EMI, easier thermal management
•
A must for very high frequency operation,
(also medium frequency at high power levels)
•
Usually involves compromises in conduction loss,
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Relationship Between Efficiency
and Power Density
0.8 0.82 0.84 0.86 0.88 0.9 0.92 0.94 0.96 0 50 100 150 200 250 300 350 400 450 500 Power Rating 20 loss P = W 10 loss P = W Efficiency 0 8. 0 84. 0 88. 0 92. 0 96. 100 200 300 400 500 0 1 out out loss out loss P P P P P η η η = + ∴ = −
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Hard-Switching
iL iL + -+ -Vd vT vdiode iL ≈ Io iT + -+ -Vd vT vdiode iL ≈ Io iT + − gate v T v T i loss P diode i diode v ( )on ( )off sw s c c P ∝ f t⎡⎣ +t ⎤⎦7 n+ p n− ds C gd C drain-body depletion layer gs C p n + gate source drain n+
Cross-sectional view of an n-channel MOSFET
MOSFET Characteristics
Output characteristics
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MOSFET Characteristics
in V GG V G R gd C gs C f D o I( )
D gs i = f VMOSFET model valid in
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Time
0s 0.5us 1.0us 1.5us 2.0us 2.5us 3.0us 3.5us 4.0us V(M1:d)/4 ID(M1)*2 V(R2:2) V(V3:+) -10 0 10 20 0 V1 50V 80 D2 I3 1A R2 25.0 M1 IRF150 R3 1m L2 40nH
Simulation of Hard Switching Converters
DS v gate input D i GS v Ideal diode IRF150
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Simulation of Hard Switching Converters
• Diode reverse recovery
Time
30.9500us 31.0000us 31.0500us 31.1000us
30.9154us 31.1299us -I(R3) V(M1:1)/3 V(M1:2) I(I1) 0 20.0 38.5 Time
32.95us 33.00us 33.05us 33.10us 33.15us 33.20us 33.25us 33.30us 33.34us -I(R3) V(M1:1)/3 V(M1:2) I(I1) 0 20.0 38.5 V1 100 R2 10 M1 MT B20N 20E V4 TD = 1u TF = 1n PW = 2u PER = {1/fs} V1 = 0 TR = 1n V2 = 15 PARAMETERS: fs = 100k R_LOAD = 1 I1 5A MU R 2020R D5 MTB20N20E MUR2020R Time
30.0us 30.4us 30.8us 31.2us 31.6us 32.0us 32.4us 32.8us 33.2us 33.6us 34.0us -I(R3) V(M1:1)/2 V(M1:2) I(I1) 0 20 40 -10 55 ds v gs v ds i o I ds v o I gs v ds i ds v ds i Io gs v
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Problems of Hard-Switching
Possible Solutions (combination)
• Snubbers to reduce di/dt and dv/dt
• Circuit layout to reduce stray inductances
• Gate drive
• Soft switching to achieve ZVS and/or ZCS
Þ usually no change in losses (unless loss recovery)
Þ circuit layout
Þ turn on / off speeds
• Switching losses
• Device stress, thermal management
• EMI due to high di/dt and dv/dt
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Snubbers
•
Passive components (R, L, C) and a diode to shape
switching trajectories
Turn-on snubber (seldom used)
i t V L t T d s ( )= • low di/dt
• lower turn-on losses in the device • low reverse recovery current
Þ At turn-on
Þ Price to be paid at turn-off
• 1/2 LI2 energy dissipated during off interval
• off interval > 2 to 3 times LS /RS time constant • switch voltage rating increases by RS IO
iT Ls Rs Io + - vT t Vd vT iT t 0 0 iT Ls Rs Io + - vT t Vd vT iT t 0 0
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Turn-off Snubbers
At turn-off
• while builds up
• switch turn-off loss decreases
• lower dv/dt iT Io iC S iC DS S = − ( flows through ) Issues at turn-on • 1/2 CV2 energy dissipated in R S and switch
• switch current rating increases by
• ON interval > 2 to 3 times RS CS time constant
vT Vd / RS iT Io + -vT CS RS Vd DS iCS iT Io + -vT CS RS Vd DS iCS vT iT Io Vd 0 CS 1 CS 2 CS 3 0 CS CS CS 3 > 2 > 1 CS=0 vT iT Io Vd 0 CS 1 CS 2 CS 3 0 CS CS CS 3 > 2 > 1 CS=0
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Soft-Switching
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ZVS (Zero Voltage Switching)
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ZCS (Zero Current Switching)
Advantages
- Lower losses (may be !)
- Low EMI (may be !)
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ZVS (Zero Voltage Switching)
Turn OFF Turn ON
• Switch voltage brought to zero before gate voltage is applied
• Ideal, zero-loss transition
• Low-loss transition
• Parallel capacitor as a loss-less snubber
• Preferred scheme for very high frequency applications using MOSFETs
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ZCS (Zero Current Switching)
Best suited for converters with IGBTs due to tail current at turn-off
• Switch current brought to zero before gate voltage is removed
• Ideal, zero-loss transition Turn OFF
Turn ON
• Low-loss transition
• Series inductor as a loss-less snubber
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ZVS and Hard-Switched Waveforms
Zero-voltage switched Hard-switched
gate source v − drain source v − 12V − 12V gate source v − drain source v − 0V 0V 12V −
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An Example: Zero Voltage Transition (ZVT)
At t = 0, T+ is turned off ( ) ( ) 0 0 0 -C d C v v V + = = - d C C v + +v =V d V + + − − Vo T+ T− D+ D− L L i C+ -C C i + -C i A
Synchronous Buck Converter
L
i
19 - d C C Since v + +v =V 0 -C C s s dv dv C C dt dt + + = 0 -C C i + i ∴ + = 0 -C d C v v V + ∴ = = 0 d V - L C C Also, i + - i =i 2 -L C C i i + -i ∴ = =
• At the end of this charge/discharge interval, positive iL is carried by
• Subsequently, is turned on; iL must reverse direction D− T− d V + + − − Vo T+ T− D+ D− L L i s C+ -s C C i + -C i A
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Zero Voltage Transition
d V + + − − Vo T+ T− D+ D− L L i s C+ -s C C i + -C i A Conducting Devices 0 t 0 ’ t t0" t1 t1’ t2 t3 d V o V L i T+ D− T− None None D+ T+ None t t
( )
a v t 0 0 ( ) A v t21
Time
9us 10us 11us 12us 13us 14us 15us 16us 17us V(M2:d)/2 ID(M2)*2 V(M2:g) I(L1)*2 V(V8:+) -20 -10 0 10 20 0 L1 20uH IC = 2A V1 21V C2 1000uF IC = 10V M1 IRF150 M2 IRF150 V8 TD = {TDLY2} V7 TD = {TDLY1} R7 25 R8 25 PARAMETERS: PulseWidth = 4.5us Period = 10us TDLY1 = 5.5us TDLY2 = 0.5us R6 10.0
Simulation of a ZVT Buck Converter
DS v inputgate D i GS v L i ZVT_buck.opj
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Classification of
Soft-Switching Schemes
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Load Resonant Converters
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Converters with Resonant Switches (Quasi-
resonant, Multi-resonant)
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Resonant Transition Converters
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Makes use of switch capacitances and transformer leakage inductance and magnetizing current
Phase Shift Controlled
Full-Bridge Converter (ZVT)
TA+ TA− TB− TB+ Db+ Db− Da− Da+ + − d V A Io B a b• Poles A & B switched at nearly 50% duty-cycle
• Output voltage regulation is achieved by phase modulating the two pole outputs
48 TA+ TA− TB− TB+ Db+ Db − Da− Da+ + − 2 d V o I A B a b + − 2 d V DA+ DA− DB− DB+ lT L 0 ficticious iL + − in V iAB + −vAB
Switching waveforms
In pole A AB v =0 A A T − to T + ⇒ +Vd AB v =0 A A T + to T − ⇒ d -V In pole B AB d B B T − to T + ⇒ v = +V AB d B B T + to T − ⇒ v = -V 0 0 AB v B v A v AB i t49
Transitions - Pole B
T to T B− B+ 0 AB d v = +V L o i stays at I • • 0 AB d v = -V • • i stays at - IL o TA+ TB− TB+ Db− Da+ + − Io A B a b d V L i AB v AB i - + B B T to T + -B B T to T t50
Transitions - Pole A
0 AB A A T + to T − ⇒ v = d -V• All four diodes conduct
• Leakage inductance resonates with switch capacitance
• Determination of Tdel critical for ZVS design
• Load dependent ZVS Db− Da+ L i TB+ + − o I A B a b d V TA− TA+ AB v AB i + -A A T to T t
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Methods to increase ZVS range
• Use of external series inductor
Disadvantages Loss of volt-sec
higher turns-ratio higher
conduction loss VA ratingsincreased
Load dependent ZVS + − Vin + − Vo A B iAB Lo Lseries + − vrect iAB vAB 0 left-leg vrect
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Use of magnetizing current
Disadvantages
higher conduction loss due to
• peak circulating current
• current through right-leg
MOSFETs
• peak magnetizing current independent of Vin
iload + imag imag
A B + − Vin imag vAB left leg
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Design of other parameters like Lo, Co, transformer etc identical to hard switched PWM
Factors Affecting ZVS
Capacitance across MOSFETs – internal and external Leakage inductance
Delay time
Magnetizing current ZVS Load Range
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Designing for ZVS
(
)
( )
2 eq ds in mag _ pk refl ds L v V I I sin t C ω = − + 1 2 L Ceq ds ω π =(
)
1 2 eqmag _ pk refl in,max
ds L . I I V C + ≥ 2 2 2 delay eq ds . T = π L . C Conditions for ZVS
MOSFET voltage during critical turn-on transition ds v t 2 2 LLk Cds π
55 A Possible Design Approach Using MathCAD
• Sweep for all practical values of
• •
• Calculate total losses. Iterate for different ZVS ranges
ds
C - based on limiting voltage rise during turn-off
delay
T - as a percentage of switching period
mag,pk lk
Calculate required I and L for each set
Calculate switch peak current and RMS current
Turn-off loss Conduction loss
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