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7/31/2019 Power Correction Circuit Theory
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Circuit Theory of Power Factor Correction
C. K. Tse
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C. K. Tse: Circuit Theory of PFC 2
Contents
Novel concept: No.
New theory: No.
What do we do here?
We will re-examine the concept of power factor correction,
starting from the basics of circuit theory. You wont learn any new thing, but hopefully somethinguseful in reinforcing your practical intuition.
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C. K. Tse: Circuit Theory of PFC 3
Introduction Efficient and compact power supplies are not
priceless.
They present themselves as nonlinear loads to themains, drawing current of distorted waveforms;
The generate noise that interferes other equipment and
the environment
Quantitative measures of power quality Power factor / harmonic distortions
Radiated and conducted EMI
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C. K. Tse: Circuit Theory of PFC 4
Power FactorOld concept of renewed interest
p.f. = Actual PowerVIProduct
= (displacement factor)(distortion factor)
Phase shift between v and i Harmonic contents in i
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C. K. Tse: Circuit Theory of PFC 5
Power Factor CorrectionPower converters are required to present themselves
as linear resistance to the supply voltage. If the input
voltage, v, is a sine wave, so is the input current, i.
+
Rv
iLinear resistor
Technique:
Power
Factor
Correction
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C. K. Tse: Circuit Theory of PFC 6
Power Converters Fundamentals Composed of inductors and switches as seen from the
mains;
Operating with switches turned on and off at a frequencymuch higher than 50 Hz.
The question is:
How to make the converter
look resistive?
v
converterR
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C. K. Tse: Circuit Theory of PFC 7
Hints The converter does not need to be resistive for all
frequencies.
If a filter is already there to remove switching frequencyripples, the converter needs only be resistive at lowfrequencies.
Afterall, power factor correction is a low-frequencyrequirement.
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C. K. Tse: Circuit Theory of PFC 8
Destruction of Dynamics
Inductors cannot (are not allowed to) have jump current
Capacitors cannot (are not allowed to) have jump voltage
Fundamental Properties
current is forced to
zero periodically
open
voltage forced to
zero periodically
closed
+
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C. K. Tse: Circuit Theory of PFC 9
Zero-order Inductors/Capacitors Inductors forming a cutset with open switch(es) and/or current source(s)periodically
Capacitors forming a loop with closed switch(es) and/or voltagessource(s) periodically
open closed
+
+ |
Zero-order elements
inductor current
iL
= 0 periodically no dynamics!
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C. K. Tse: Circuit Theory of PFC 10
Devoid of DynamicsZero-order elements (L0 or C0) obviously do not store energyin a cycle, and hence are devoid of low-frequency dynamics.They can be considered as being resistive in the low-frequency range.
open closed
+
+ |
Zero-order elements
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C. K. Tse: Circuit Theory of PFC 11
First IdeaIf the converter contains only zero-order elements; and
the input does not see the output at all times,
then the converter will look resistive to the input.Thus, we can make a PFC converter from this idea.
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C. K. Tse: Circuit Theory of PFC 12
The Perfect SolutionConsider a flyback or buck-boost converter.
First, we can see that the input
never see the output.
So, if we make the inductor
zero-order by operating it in
DCM, we have a resistive input.
DCM operation
forming cutset with open
switches periodically
Rin =2L
D2T
Applying simple averaging, input resistance is
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C. K. Tse: Circuit Theory of PFC 13
A Not-So-Perfect SolutionConsider a boost converter.
Observe that the input
sometimes see the output!!
Even if we make the inductor
zero-order by operating it in
DCM, we dont precisely have a
resistive input.
forming cutset with open
switches periodically by
DCM operation
Rin =2L
D2T
1-Vin
Vo
Applying simple averaging, input resistance is
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C. K. Tse: Circuit Theory of PFC 14
Perfecting It!Consider a boost converter again. forming cutset with openswitches periodically by
DCM operation
Rin =2L
D2T
1-Vin
Vo
variable
IfD is reserved for other purposes, the Tmust be varied to achieve
perfect PFC, as in SSIPP*. (See Chow et al., 1997)It was also shown (Redl et al. and others) that even if no control is used,
the power factor attained is still pretty goodgood enough!
Feedback
feedforward
*SSIPPsingle-stage single-switch isolated PFC power supply
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C. K. Tse: Circuit Theory of PFC 15
What do we know now? The DCM buck-boost or flyback converter satisfies the basic criteria of a
perfect PFC. It thus naturally gives a good p.f.
The DCM boost and buck converters are not-so-perfect, but can theoretically
be perfected via feedback/feedforward.
The DCM boost converter is preferred for its relatively better efficiency.
Even under no control, the DCM boost converter has a pretty good p.f.
The DCM buck converter is not preferred for its high peak current, and itsuffers from the low voltage blackout (because it is a buck)!
Basic Criteria:
Other Practical Considerations:
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C. K. Tse: Circuit Theory of PFC 16
Other PossibilitiesOur fundamental criterion is
Destruction of Dynamics of L and C!
For voltage converters, the main constituent is the switching L.
Therefore, our basic wish is to destroy the dynamics of the L in
the converter.
We have shown how this destruction can be done by DCM
operation. What else can we do?
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C. K. Tse: Circuit Theory of PFC 17
Direct Destruction
Using direct current-programming, we can destroy the
dynamics of the L. (The idea is that if we make the current
dependent on the output voltage, it is no longer an independent
variable, hence it is devoid of dynamics!)
Specifically, we program the current of L such that it assumes
the wave shape that we want.
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C. K. Tse: Circuit Theory of PFC 18
Second Idea
CCM operation of the boost
converter.
Direct current programming such
that its average (ripple removed)
waveshape follows the input.
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C. K. Tse: Circuit Theory of PFC 19
Standard IC Implementation
e.g., ACM PFC IC controller (see Wong, Tse & Tang in PESC2004)
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C. K. Tse: Circuit Theory of PFC 20
Other Ideas
We have considered zero-order L.
How about zero-order C?
The problem (of course) is the basic restriction of
- the supply being a voltage
- the usual load requiring a voltage
(Thats why all converters are switching inductors in practice.)
Theoretically, switching capacitors are never excluded!
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C. K. Tse: Circuit Theory of PFC 21
Duality Derivation
dual of
DCM
buck
dual of
DCM
buck-
boost
dual of
DCM
boost
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C. K. Tse: Circuit Theory of PFC 22
e.g. Duality Derived SSIPP
SSIPP based on boost + buck cascadeexact dual
For detailed analysis and experiments, seeC. K. Tse, Y. M. Lai, R. J. Xie and M. H. L. Chow, Application of Duality Principle to Synthesis of
Single-Stage Power-Factor-Correction Voltage Regulators,International Journal of Circuit Theory
and Applications, vol. 31, no. 6, pp. 555-570, November 2003.
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C. K. Tse: Circuit Theory of PFC 23
Many other possibilities exist within
this theoretical framework!
Let the engineers create their own circuits.
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C. K. Tse: Circuit Theory of PFC 24
Practical PFC System
Always require tightly regulated DC output, in addition to
PFC.
Can one converter do the jobs of PFC and tight outputregulation?
No!
because we need a low-freq power buffer!
viniin sin2wm t
Po
PFC converter
with tightly
regulated output
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C. K. Tse: Circuit Theory of PFC 25
Power Buffer
In general we need a power buffer to achieve PFC and tight
output regulation simultaneously.
3-port model How many basic converters dowe need?
Answer: TWO.(For a rigorous proof, see
C. K. Tse and M. H. L. Chow,
Theoretical study of SwitchingConverters with Power Factor
Correction and Voltage Regulation,
IEEE Transactions on Circuits and
Systems I, vol. 47, no. 7, pp. 1047-
1055, July 2000.)
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C. K. Tse: Circuit Theory of PFC 26
Two is enough!
We need two converters (arranged suitably, of course).
In fact, the so-called single-stage PFC regulator has two
converter stages, strictly speaking. For example, the SSIPPis a boost converter plus a buck converter.
SSIPP by Redl et al.
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C. K. Tse: Circuit Theory of PFC 27
A Different Question
Probably, the question of interest to the engineers isHOW THE TWO
CONVERTERS ARE POSSIBLY ARRANGED?
Best known configuration:
PFC dc/dc
cascade structure
low-freq power buffer
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C. K. Tse: Circuit Theory of PFC 29
Power Processing
Lets start from the basics again.
In what ways power can flow within
the 3-port model?
I II III
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C. K. Tse: Circuit Theory of PFC 30
Power ProcessingLets try fitting in the three types of flows.
Type I and Type I
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C. K. Tse: Circuit Theory of PFC 31
Power ProcessingAnother try!
Type I , Type II
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C. K. Tse: Circuit Theory of PFC 32
Power ProcessingAnother try!
Type I , Type III
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C. K. Tse: Circuit Theory of PFC 33
Power ProcessingAnother try!
Type II , Type III
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C. K. Tse: Circuit Theory of PFC 34
Power Processing PossibilitiesTo fulfill the power flow conditions of the 3-port model, we
have 4 power flow possibilities.
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C. K. Tse: Circuit Theory of PFC 35
Completing the StructureFinally, we place 1 converter to each path.
1 2 12
and 2 others!
12
and 2 others!
12
and 8 others!
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C. K. Tse: Circuit Theory of PFC 36
The Sixteen ConfigurationsFitting in the two basic converters, we clearly see 16 possible structures.
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C. K. Tse: Circuit Theory of PFC 37
Theoretical EfficiencyWe can theoretically compare the efficiencies of the 16 structures.
Obviously, the cascade (type I-I) is the poorest, and the others are always
better since power is not doubly processed.
For example, consider the I-IIA structure.
Suppose kis the ratio of power split.
efficiency = kh1h2 + (1- k)h2
= h1h2 + (1- k)h1(1-h2)
> h1
h
2
k
1k
We shall see that this kis a very important parameter. Ifkis too large, the circuit
resembles the cascade structure, hence no efficiency advantage. But if it is too
small, P.F. degrades.
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C. K. Tse: Circuit Theory of PFC 38
Theoretical EfficiencyWe can theoretically compare the efficiencies of the 16 structures.
Obviously, the cascade (type I-I) is the poorest, and the others are always
better since power is not doubly processed.
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C. K. Tse: Circuit Theory of PFC 39
Comparing EfficiencyNote:
I dont mean the above efficiency comparison is absolute! That will
always put me in endless debate! You may have different efficiency
optimization schemes for different stages, and in different forms.
So, why should I bother here?
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C. K. Tse: Circuit Theory of PFC 40
SynthesisThe most important problem is HOW TO CREATE CIRCUITS.
We consider the following basic converters to be inserted in any of the 16
structures.
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C. K. Tse: Circuit Theory of PFC 41
Synthesis ProcedureFor a detailed procedure, see
C. K. Tse, M. H. L. Chow and M. K. H. Cheung, A Family of PFC Voltage Regulator
Configurations with Reduced Redundant Power Processing,IEEE Transactions on Power
Electronics, vol. 16, no. 6, pp. 794-802, November 2001. (IEEE Transactions Best Paper
Award Winner)
In brief, we insert
suitable converters in
the respective
positions (guided by
certain circuit rules),
and we will end upwith a PFC voltage
regulator of the
desired
characteristics.
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C. K. Tse: Circuit Theory of PFC 42
The ChoiceIt turns out that not all converters can be inserted. No free choice! This
table shows the allowable configurations.
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C. K. Tse: Circuit Theory of PFC 43
Synthesis ExamplesType I-IIB using a buck-boost and a buck converter.
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C. K. Tse: Circuit Theory of PFC 44
Synthesis ExamplesType I-IIA using a buck-boost and a buck converter.
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C. K. Tse: Circuit Theory of PFC 45
and moreType I-IIIB using buck-boost converters. Type I-IIIA using a buck-boost and
a buck converter.
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C. K. Tse: Circuit Theory of PFC 46
Control Problem
From formal theoretical study, we conclude that
In general we need TWO independent controls for
full power control of two stages.
For CCM-CCM, two duty cycles should be used.
For DCM-CCM or CCM-DCM, frequency and duty
cycle can be used
Thus, single switch is possible if controls off
and dare properly designed
Reasonable performance if only dcontrol is
used for cascade structure (shown by Redl et
al. 1994)
PFC
(DCM or CCM)
dc/dc
(DCM or CCM)
SSIPP by Redl et al.(DCM-CCM or DCM-DCM)
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C. K. Tse: Circuit Theory of PFC 47
Practical DesignVarious configurations tested experimentally, e.g., see C. K. Tse, M. H. L. Chow and M. K. H.Cheung, A Family of PFC Voltage Regulator Configurations with Reduced Redundant Power
Processing,IEEE Transactions on Power Electronics, vol. 16, no. 6, pp. 794-802, November 2001.
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C. K. Tse: Circuit Theory of PFC 49
Open Unsolved ProblemsWe have seen the comparison of the cascade (type
I-I) and non-cascade (all other types) structures.
All non-cascade structures involve a power split.
The design parameter is k.
We observe that there is a trade off of PFC
performance and efficiency. We mentioned (in
slide #37) that the power split ratio kis important!
Can we optimize the design? What kgives best
trade-off?
k
1k
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C. K. Tse: Circuit Theory of PFC 50
Final ConclusionI probably have not said anything new.
The point is that power factor correction and most other concepts are
probably not new from the point of view of formal circuit theory. The
question is whether how the problem can be best understood from the
basics, and then and tackled in the best possible way.
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C. K. Tse: Circuit Theory of PFC 51
References1. C. K. Tse, Zero-order switching networks and their applications to power
factor correction in switching converters,IEEE Transactions on Circuits
and Systems Part I, vol. 44, no. 8, pp. 667-675, August 1997.
2. C. K. Tse and M. H. L. Chow, Theoretical study of Switching Converters
with Power Factor Correction and Voltage Regulation,IEEE Transactions
on Circuits and Systems I, vol. 47, no. 7, pp. 1047-1055, July 2000.
3. C. K. Tse, M. H. L. Chow and M. K. H. Cheung, A Family of PFC Voltage
Regulator Configurations with Reduced Redundant Power Processing,IEEE
Transactions on Power Electronics, vol. 16, no. 6, pp. 794-802, November
2001. (IEEE Transactions Best Paper Award Winner)
4. C. K. Tse, Y. M. Lai, R. J. Xie and M. H. L. Chow, Application of DualityPrinciple to Synthesis of Single-Stage Power-Factor-Correction Voltage
Regulators,International Journal of Circuit Theory and Applications, vol.
31, no. 6, pp. 555-570, November 2003.
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C. K. Tse: Circuit Theory of PFC 52
All we need to know we learnt in kindergarten.