Power Elec Notes 07a Intro to Dc-dc Converters

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1Introduction to DC/DC Converters© M. T. Thompson, 2008

Power Electronics Notes 07AIntroduction to DC/DC Converters

Portions of these notes excerpted from the CD ROM accompanying Mohan, Undeland and Robbins, Power Electronics Converters, Applications and Design, 3d edition, John Wiley 2003Other notes © Marc Thompson, 2008

Marc T. Thompson, Ph.D.Thompson Consulting, Inc.

9 Jacob Gates RoadHarvard, MA 01451

Phone: (978) 456-7722 Fax: (888) 538-3824

Email: marctt@thompsonrd.comWeb: http://www.thompsonrd.com

2Introduction to DC/DC Converters© M. T. Thompson, 2008

Summary

• Non-isolated (i.e. no transformer) DC/DC converters• Step down (buck)• Step up (boost)• Buck-boost• Cuk converter• SEPIC

• Full-bridge• Comparison of DC/DC converters

3Introduction to DC/DC Converters© M. T. Thompson, 2008

Block Diagram of Typical AC Input, Regulated DC Output System

• Typically, a power supply front end has uncontrolled full-wave diode rectifier, followed by a bus (“hold-up”) capacitor, followed by a DC/DC converter with active feedback control

4Introduction to DC/DC Converters© M. T. Thompson, 2008

Offline Flyback Converter

Reference: http://www.st.com/stonline/products/literature/an/7310.pdf

5Introduction to DC/DC Converters© M. T. Thompson, 2008

Some Real-World Design Issues that We’ll Get to Later On in the Term

6Introduction to DC/DC Converters© M. T. Thompson, 2008

Stepping Down a DC Voltage

• In this example, the average value of the output voltage = DVin where D is the DUTY CYCLE in PWM (pulse-width modulation) control• D = ton/Ts, the fraction of the total switching cycle that the switch is ON

7Introduction to DC/DC Converters© M. T. Thompson, 2008

Frequency Spectrum of Vo

fs= 1/TsVo = Vd D

• The output voltage contains switching harmonics

8Introduction to DC/DC Converters© M. T. Thompson, 2008

Adding a Lowpass Filter to the Buck Converter

• The goal of the lowpass filter LC is to pass the DC component, while attenuating the switching components• As frequency increases, XL increases and XC decreases

9Introduction to DC/DC Converters© M. T. Thompson, 2008

Adding a Lowpass Filter to the Buck Converter

• The corner frequency must be lower than the switching frequency to attenuate the switching harmonics.

• Corner frequency:

-40 dB/decade

10Introduction to DC/DC Converters© M. T. Thompson, 2008

Step-Down (Buck) Converter

• Diode needed to provide current path for output current when switch is OFF

11Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck Converter in Continuous Conduction• In periodic steady state, inductor current flows continuously• Waveform here are for buck in continuous conduction mode; note that inductor current never decays to zero• In discontinuous conduction mode, there are 3 states

12Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck Converter: PSPICE Circuit

• Circuit shown: fsw = 200 kHz, D = 0.5

13Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck Converter: Startup Waveforms• These waveforms are shown for a constant duty cycle of D = 0.5 during startup • Note large overshoot on output voltage and inductor current

14Introduction to DC/DC Converters© M. T. Thompson, 2008

Same Circuit --- PSIM Simulation

15Introduction to DC/DC Converters© M. T. Thompson, 2008

Same Circuit --- PSIM Simulation

16Introduction to DC/DC Converters© M. T. Thompson, 2008

Analysis for DC/DC Converters in Continuous Conduction and Steady State

• In steady state, the inductor current returns to the same value every switching cycle, or every T seconds• Therefore, the inductor ripple current UP equals ripple DOWN• Several assumptions to simplify analysis:

• Periodic steady state --- all startup transients have died out• Small ripple --- ripple is small compared to average values. For instance, output voltage ripple is small compared to the DC value

17Introduction to DC/DC Converters© M. T. Thompson, 2008

Inductor Voltage and Current• Remember that in an inductor:

dt

diLv L

L

18Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck Converter in Continuous Conduction

V o

DiL

LV cc

v c

+

-

C R

• In continuous conduction, buck converter has 2 states --- switch OPEN and switch CLOSED.• We can solve for output voltage by focusing on inductor Volt-second balance

19Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck Converter in Continuous Conduction

V o

DiL

LV cc

v c

+

-

C R

V o

iL

LV cc

v c

+

-

C R

V o

iL

L

v c

+

-

Switch closed (for time DT) Switch open (for time (1-D)T)

di

dt

V v

LL CC o

di

dt

v

LL o

20Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck Converter in Continuous Conduction

• The inductor ripple current UP equals ripple DOWN

• We already knew this result by inspection, but this methodology of inductor Volt-second balance can be used to evaluate other more complicated DC/DC converters, such as the boost, buck-boost, etc.

( ) ( )V V DT

L

V D T

LV DV

CC o o

o CC

10

21Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck Converter in Continuous Conduction --- Idealized Switching Waveforms

• Idealized because we assume that switches and diodes turn on and off with zero risetime

22Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck Converter: Waveforms at the Boundary of Cont./Discont. Conduction

• ILB = critical current below which inductor current becomes discontinuous

23Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck Converter: Discontinuous Conduction Mode• Steady state; inductor current discontinuous (i.e. it goes zero for a time)• Note that output voltage depends on load current

max,

2

2

25.0

LB

od

o

I

ID

D

V

V

24Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck Converter: Capacitor Current Ripple

• Continuous conduction mode

25Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck Converter: Output Voltage Ripple

• ESR is assumed to be zero; continuous conduction mode

26Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck Converter: Output Voltage Ripple

• ESR is assumed to be zero

Lf

DV

L

TDVi

sw

ooppL

)1()1(,

Lf

DViTQ

sw

oppL

2

,

8

)1(

222

1

LCf

DV

C

Qv

sw

oppo 2, 8

)1(

27Introduction to DC/DC Converters© M. T. Thompson, 2008

Example 1: Buck Converter Calculations

• Shown for SPICE example with fsw = 200 kHz, D = 0.5, L = 33 µH, C = 10 µF, Io = 1A

ALf

DVi

sw

oppL 38.0

)1033)(102(

)5.01)(5()1(65,

mVLCf

DV

C

Qv

sw

oppo 24

)1010)(1033()102(8

)5.01)(5(

8

)1(66252,

28Introduction to DC/DC Converters© M. T. Thompson, 2008

Example 1: Buck in Periodic Steady State

• Analysis shows inductor ripple = 0.38 A-pp, output voltage ripple = 24 mV-pp, confirmed by SPICE

29Introduction to DC/DC Converters© M. T. Thompson, 2008

Step-Up (Boost) DC-DC Converter

• Output voltage is greater than the input, with the same polarity

30Introduction to DC/DC Converters© M. T. Thompson, 2008

Boost Converter Waveforms in CCM• Continuous conduction mode (CCM)

Switch closed:

di

dt

V

LL CC

Switch open:

di

dt

V v

LL CC o

Inductor Volt-second balance:V DT

L

V V D T

L

VV

D

CC CC o

oCC

( )( )10

1

31Introduction to DC/DC Converters© M. T. Thompson, 2008

Boost Converter: Discontinuous Conduction

• Occurs at light loads

32Introduction to DC/DC Converters© M. T. Thompson, 2008

Boost Converter: Effect of Parasitics• The duty-ratio D is generally limited before the parasitic effects become significant• As D gets big, input current gets very large (think about power balance….); the voltage drop in inductor and switch cause efficiency to suffer

33Introduction to DC/DC Converters© M. T. Thompson, 2008

Boost Converter Output Ripple• ESR is assumed to be zero• Assume that all the ripple component of diode current flows through capacitor; DC component flows through resistor

34Introduction to DC/DC Converters© M. T. Thompson, 2008

Boost Converter --- PSIM Simulation• What is the output voltage?

35Introduction to DC/DC Converters© M. T. Thompson, 2008

Boost Converter --- PSIM Simulation• Vo = Vi/(1-D) in continuous conduction

Output voltage during startup

36Introduction to DC/DC Converters© M. T. Thompson, 2008

Boost Converter --- PSIM Simulation• Note that inductor current I(RL1) never decays to zero, so we’re in continuous conduction

37Introduction to DC/DC Converters© M. T. Thompson, 2008

Example 2: Boost Converter Example• Mohan, Example 7-1• Boost converter on the edge of discontinuous conduction• Vi = 12V, D = 0.75, Vo = 48V, Po = 120W

38Introduction to DC/DC Converters© M. T. Thompson, 2008

Example 2: Boost Converter Example

Output voltage ripple

Inductor ripple current

39Introduction to DC/DC Converters© M. T. Thompson, 2008

Step-Down/Up (Buck-Boost) Converter

• The output voltage can be higher or lower than the input voltage

40Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck-Boost Converter: Waveforms• Continuous conduction mode

Switch closed:

di

dt

V

LL CC

Switch open:

di

dt

v

LL o

Inductor Volt-second balance:

D

DVV

L

TDV

L

DTV

CCo

oCC

1

0)1(

41Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck-Boost: Limits of Cont./Discont. Conduction

• The output voltage is held constant

42Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck-Boost: Discontinuous Conduction• This occurs at light loads

43Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck-Boost Converter: Effect of Parasitics

• The duty-ratio is limited to avoid these parasitic effects from becoming significant

44Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck-Boost Converter: Output Voltage Ripple

• ESR is assumed to be zero

45Introduction to DC/DC Converters© M. T. Thompson, 2008

Example 3: Buck-Boost Converter: Simulation

• Vo should be -10V after startup transient dies out

46Introduction to DC/DC Converters© M. T. Thompson, 2008

Example 3: Buck-Boost Converter: Simulation

• Vo should be -10V in steady-state after startup transients die out

Output voltage during startup

47Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck-Boost Converter: Simulation

• The ripple is pretty big (0.5 V pp)• Let’s increase the size of the filter capacitor by 10 --- what will happen?

48Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck-Boost Converter: Simulation

• With larger C• What has happened?

Output voltage during startup

49Introduction to DC/DC Converters© M. T. Thompson, 2008

Buck-Boost Converter: Simulation

• Note that ripple is smaller, but startup transient is slower (makes sense); LC is larger

Output voltage during startup

50Introduction to DC/DC Converters© M. T. Thompson, 2008

Cuk DC-DC Converter• The output voltage can be higher or lower than the input voltage• Capacitor C1 stores and transfers energy from input to output• When switch is ON, C1 discharges through the switch and transfers energy to the output• When switch is OFF, capacitor C1 is charged through the diode by energy from the input and L1

51Introduction to DC/DC Converters© M. T. Thompson, 2008

Cuk DC-DC Converter: Waveforms

• The capacitor voltage is assumed constant (very large)• Note phase inversion at the output

D

D

V

V

d

o

1

52Introduction to DC/DC Converters© M. T. Thompson, 2008

SEPIC Converter

• Single-ended primary inductance converter (SEPIC)• Can buck or boost the voltage• Note that output is similar to buck-boost, but without a phase inversion• This circuit is useful for lithium battery powered equipment

D

D

V

V

d

o

1

53Introduction to DC/DC Converters© M. T. Thompson, 2008

SEPIC Converter

• Circuits for 2 different switching states

Reference: National Semiconductor, Application Note AN-1484, “Designing a SEPIC Converter”

54Introduction to DC/DC Converters© M. T. Thompson, 2008

SEPIC Converter --- Example

• Example from application note

Reference: National Semiconductor, Application Note AN-1484, “Designing a SEPIC Converter”

55Introduction to DC/DC Converters© M. T. Thompson, 2008

SEPIC Converter

56Introduction to DC/DC Converters© M. T. Thompson, 2008

SEPIC Converter

Output voltage ripple

57Introduction to DC/DC Converters© M. T. Thompson, 2008

Converter for DC-Motor Drives• Four quadrant operation is possible• For:

• DC motor drives• DC to AC inverters for UPS

58Introduction to DC/DC Converters© M. T. Thompson, 2008

Switch Utilization in DC-DC Converters

• It varies significantly in various converters• PT = VTIT where VT and IT are peak switch voltage and current• In direct converters (buck and boost) switch utilization is good; in indirect converter (buck-boost and Cuk) switch utilization is poor

59Introduction to DC/DC Converters© M. T. Thompson, 2008

Equivalent Circuits in DC-DC Converters• Replacing inductors and capacitors by current and voltage sources, respectively

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