PFC1 - Advanced Power Factor Correction

Advanced Power Factor Correction
Agenda
• Introduction
ƒ Basic solutions for power factor correction
ƒ New needs to address
• Interleaved PFC
ƒ Basic characteristics
ƒ A discrete solution
ƒ Performance
• Bridgeless PFC
ƒ
ƒ
ƒ
ƒ
Why should we care of the input bridge?
Main solutions
Ivo Barbi solution
Performance of a wide mains, 800 W application
• Conclusion
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2
Agenda
• Introduction
ƒ Basic solutions for power factor correction
ƒ New needs to address
• Interleaved PFC
ƒ Basic characteristics
ƒ A discrete solution
ƒ Performance
• Bridgeless PFC
ƒ
ƒ
ƒ
ƒ
Why should we care of the input bridge?
Main solutions
Ivo Barbi solution
Performance of a wide mains, 800 W application
• Conclusion
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3
Why Implement PFC?
Vin (t ) = 2 ⋅ Vin( rms ) ⋅ sin(ω t )
Iin (t ) = ?
Ac line
• The mains utility provides a sinusoidal voltage Vin(t).
• The shape and phase of Iin(t) depend on the load.
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AC Line Rectification Leads to
Current Spikes…
Rectifiers
Cbulk is refueled
when Vin(t) > Vout
Converter
VIN
Ac
Line
Bulk
Storage
Capacitor
Load
3
2
1
Iin(t)
Vin(t)
High current
spike!
• Only the fundamental component produces real power
• Harmonic currents circulate uselessly (reactive power)
• The line rms current increases
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Too High rms Currents!...
• High rms currents reduce outlet capability
n°1
ƒ Pin(avg) = 119 W, Vin(rms) = 85 V
ƒ Iin(rms) = 2.5 A
n°2
ƒ Pin(avg) = 119 W, Vin(rms) = 85 V
ƒ Iin(rms) = 1.4 A
PF = 0.56
Same
power
(W)
PF = 1.00
n°1
n°2
16/2.5 = 6 monitors
16/1.4 = 11 resistors
Iin( rms ) =
(Iin(rms))max = 16 A
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Pin(avg )
Vin( rms ) ⋅ PF
Power Factor Standard
Class
ClassCC
YES
Lighting
Lighting
Equipment?
Equipment?
IEC61000-3-2
Class
ClassBB
YES
NO
NO
Portable
PortableTool?
Tool?
NO
Special
Special
Waveform
Waveform
P<=600W?
P<=600W?
YES
YES
Motor
Motor
Equipment?
Equipment?
NO
NO
Three
ThreePhase
Phase
Equipment?
Equipment?
Class
ClassDD
YES
Class
ClassAA
Mandatory for
PC, TV sets
Monitors
P > 75 W
• The standard specifies a maximum level up to harmonic 39
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Need for a PFC Stage
PFC Stage
Diode Bridge
Power Supply
+
AC
Line
Controller
Controller
IN
Bulk
Capacitor
LOAD
LOAD
-
Current
reference
Icoil,pk
Iline(t)
• A boost pre-converter draws a sinusoidal current from the
line to provide a dc voltage (bulk voltage)
• The current within the coil is made sinusoidal by:
– Forcing it to follow a sinusoidal reference (current mode)
– Controlling the duty-cycle appropriately (voltage mode)
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Operating Modes Overview
• ON Semiconductor offers solutions for three modes
Operating Mode
IL
IL
IL
Tclamp
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Tclamp
Main Feature
Continuous
Conduction Mode
(CCM)
Always hard-switching
Inductor value is largest
Minimized rms current
e.g.: NCP1654
Critical conduction
Mode (CrM)
Large rms current
Switching frequency is not
fixed
e.g.: NCP1606
Frequency Clamped
Critical Conduction
Mode (FCCrM)
Large rms current
Frequency is limited
Reduced coil inductance
e.g.: NCP1605
FCCrM: an Efficient Mode
• Frequency Clamped CrM seems the most efficient solution
• Efficiency of a 300 W, wide mains PFC has been measured:
Efficiency at 100 Vrms
NCP1605 (FCCrM)
NCP1606 (CrM)
20%
30%
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10
40%
The complete
study will be
published in the
PFC handbook
revision that will
be released in
Q1 2009.
NCP1654 (CCM)
50%
60%
70%
Output Load
80%
90%
100%
New Needs to Address
• High efficiency for ATX power supplies:
– Efficiency is measured at:
• 20% Pout(max)
• 50% Pout(max)
• 100% Pout(max)
•
Slim LCD TVs:
– Components height is limited
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Agenda
• Introduction
ƒ Basic solutions for power factor correction
ƒ New needs to address
• Interleaved PFC
ƒ Basic characteristics
ƒ A discrete solution
ƒ Performance
• Bridgeless PFC
ƒ
ƒ
ƒ
ƒ
Why should we care of the input bridge?
Main solutions
Ivo Barbi solution
Performance of a wide mains, 800 W application
• Conclusion
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12
Interleaved PFC
• Two small PFC stages delivering (Pin(avg) / 2) in lieu of a
single big one
IL1
Ac line
Iin (t )
ID1
1
8
2
7
3
6
4
5
NCP1601
Vin (t )
EMI
Filter
IL(tot )
IL 2
ID 2
1
8
2
7
3
6
4
5
NCP1601
ID(tot )
Cbulk
Vout
LOAD
• If the two phases are out-of-phase, the resulting currents
(IL(tot)) and (ID(tot)) exhibit a dramatically reduced ripple.
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Interleaved Benefits
• More components but:
– A 150 W PFC is easier to design than a 300 W one
– Modular approach
– Two DCM PFCs look like a CCM PFC converter…
• Eases EMI filtering and reduces the output rms current
• Only interleaving of DCM PFCs will be considered
0
Iin
3
0
2
0
(Icoil)phase1
(Icoil)phase2
1
time
0
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Input Current Ripple
What is the
ripple of the
IL(tot) total input
current?
IL1
ID1
1
Ac line
Iin (t )
8
2
7
3
6
4
5
NCP1601
Vin (t )
EMI
Filter
IL(tot )
IL2
ID2
1
8
2
7
3
6
4
5
NCP1601
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ID(tot )
Cbulk
Vout
LOAD
Computing the Input Current Ripple
• Let’s assume that:
– Vin and the switching period are constant over few cycles
– The two branches operate in CrM
• There are two cases:
– Vin <Vout /2 (or d>0.5):
The on-times of the two phases overlap. The input
current peaks at the end of the conduction intervals.
– Vin >Vout /2 (or d<0.5):
There is no overlap but still, the input current peaks
at the end of the each conduction time
• Using
⎛
ton
Vin
=
=
−
1
d
⎜⎜
Tsw
Vout
⎝
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⎞
⎟⎟,
⎠
we can derive the current ripple
Finally,…
Vin (t ) ≤
Averaged input
current
(line current)
(
Peak Current
envelop
(
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Iin (t ) = IL(tot )
Peak to peak ripple
Valley Current
envelop
Vout
2
ΔIL(tot )
IL( tot )
)
)pp
pk
Tsw
⎛
Vin
= Iin ⋅ ⎜⎜ 1 −
⎝ Vout − Vin
v
Vout
= Iin ⋅
2 ⋅ (Vout − Vin )
Vout
2
Vin Vin ⋅ Pin(avg )
=
=
Rin
Vin( rms )2
⎞
⎟⎟
⎠
⎛
⎞
Vout
= 2 ⋅ Iin ⋅ ⎜ 1 −
⎟
⎜
⎟
V
V
4
⋅
−
(
)
out
in ⎠
⎝
(I ( ) )
L tot
Vin (t ) ≥
(
ΔIL(tot )
(I ( ) )
L tot
)pp
⎞
⎟⎟
⎠
⎛
Vout ⎞
= 2 ⋅ Iin ⋅ ⎜⎜ 1 −
⎟⎟
⋅
V
4
in ⎠
⎝
pk
(I ( ) )
L tot
⎛
V
= Iin ⋅ ⎜⎜ 2 − out
Vin
⎝
v
=
Pin(avg ) ⋅ Vout
2 ⋅ Vin( rms )2
Peak to Peak Ripple of the Input Current
( ΔIL(tot ) )pp
Iin
120
P k to pk rip ple (% )
100
⎛V
(%) vs ⎜⎜ V in
⎝ out
• The input ripple only
depends on the ratio (Vin
/Vout):
• Unlike in CCM:
⎞
⎟⎟
⎠
Ripple is 0 at
Vin = Vout / 2
80
– L plays no role
– The ripple percentage does
not depend on the load
60
40
• At low line (Vin /Vout = 0.3),
the ripple is +/-28% (at the
20
0
0
0.25
0.5
Vin/Vout
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0.75
1
sinusoid top, assuming 180°
phase shift and CrM operation)
Input Current Ripple at Low Line
• When Vin remains lower than Vout / 2, the input current looks
like that of a CCM, hysteretic PFC
• (IL(tot)) swings between two nearly sinusoidal envelops
Peak, averaged and valley current @ 90 Vrms, 320 W input
(Vout = 390 V)
Peak, valley and averaged Input
Current (A)
7
Iin(t)
6
Envelop for the peak currents
5
4
3
Envelop for the valley currents
2
1
0
0.00%
25.00%
50.00%
75.00%
time as a percentage of a period (%)
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100.00%
Input Current Ripple at High Line
• When Vin exceeds (Vout / 2), the valley current is constant!
⎛ Vout
• It equates ⎜⎜
⎝ 2 ⋅ Rin
⎞
⎟⎟ where Rin is the PFC input impedance
⎠
Peak, averaged and valley current @ 230 Vrms, 320 W input
(Vout = 390 V)
Peak, valley and averaged Input
Current (A)
3.0
Iin(t)
2.5
2.0
1.5
1.0
0.5
0.0
0.00%
Pin(avg )⋅Vout
25.00%
50.00%
75.00%
time as a percentage of a period (%)
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No ripple
when
Vin = Vout / 2
100.00%
2 ⋅ Vin( rms )2
=
Vout
2 ⋅ Rin
Line Input Current
• For each branch, somewhere within the sinusoid:
2 ⋅ IL1
Tsw
IL1
IL1
Tsw
• The sum of the two averaged, sinusoidal phases currents
gives the total line current:
Iin = IL( tot )
Tsw
2
= IL1
Tsw
+ IL 2
Tsw
• Assuming a perfect current balacing:
2 ⋅ IL1
Tsw
= 2 ⋅ IL 2
Tsw
= Iin
• The peak current in each branch is Iin(t)
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Ac Component of the Refueling Current
• The refueling current (output diode(s) current) depends on
the mode:
2.I
in
Iin
Iin
Single phase CCM
Single phase CrM
Interleaved CrM
rms value
over Tsw
rms value
over Tsw
rms value
over Tsw
Iin ⋅
Vin
Vout
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Phase 1
Phase 2
2
3
⋅ Iin
Vin
Vout
Iin
Vin
2
⋅ Iin
3
Vout
A Reduced RMS Current in the Bulk Capacitor
• Integration over the sinusoid leads to (resistive load):
Single phase CCM
PFC
Diode(s) rms
current
(ID(rms))
Single phase CrM or
FCCrM PFC
2
2
⎛P ⎞
8 2 ⋅ ⎜ out ⎟
⎝ η ⎠
3π ⋅Vin( rms ) ⋅Vout
⎛P ⎞
8 2 ⋅ ⎜ out ⎟
⎝ η ⎠ − ⎛ Pout
⎜
3π ⋅ Vin( rms ) ⋅ Vout ⎜⎝ Vout
300 W,
Vout=390V
Vin(rms)=90 V
ID(rms) = 1.9 A
IC(rms) = 1.7 A
2
⎛P ⎞
8 2 ⋅ ⎜ out ⎟
2
⎝ η ⎠
⋅
3π ⋅Vin( rms ) ⋅ Vout
3
⎛P ⎞
8 2 ⋅ ⎜ out ⎟
2
⎝ η ⎠
⋅
3
3π ⋅Vin( rms ) ⋅Vout
2
2
Capacitor
rms current
(IC(rms))
⎞
⎟⎟
⎠
2
⎛P ⎞
32 2 ⋅ ⎜ out ⎟
⎝ η ⎠ − ⎛ Pout
⎜
9π ⋅ Vin( rms ) ⋅ Vout ⎜⎝ Vout
ID(rms) = 2.2 A
IC(rms) = 2.1 A
Interleaved CrM or
FCCrM PFC
2
⎞
⎟⎟
⎠
2
⎛P ⎞
16 2 ⋅ ⎜ out ⎟
⎝ η ⎠ − ⎛ Pout
⎜
9π ⋅ Vin( rms ) ⋅ Vout ⎜⎝ Vout
ID(tot)(rms) = 1.5 A
IC(rms) = 1.3 A
• Interleaving dramatically reduces the rms currents
Î reduced losses, lower heating, increased reliability
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⎞
⎟⎟
⎠
2
Summary
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Agenda
• Introduction
ƒ Basic solutions for power factor correction
ƒ New needs to address
• Interleaved PFC
ƒ Basic characteristics
ƒ A discrete solution
ƒ Performance
• Bridgeless PFC
ƒ
ƒ
ƒ
ƒ
Why should we care of the input bridge?
Main solutions
Ivo Barbi solution
Performance of a wide mains, 800 W application
• Conclusion
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25
Interleaving: Master/Slave Approach…
• The master branch operates freely
• The slave follows with a 180° phase shift
• Main challenge: maintaining the CrM operation (no CCM,
no dead-time)
L2 < L1
Tsw
2
Tsw
2
Tsw
2
Current mode: inductor unbalance
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Tsw
2
Tsw
2
Tsw
2
Voltage mode: on-time shift
Interleaving: Independent Phases Approach…
• Each phase properly operates in CrM or FCCrM.
• The two branches interact to set the 180° phase shift
• Main challenge: to keep the proper phase shift
On-time perturbation for one phase
Tsw
2
Tsw
2
• We selected this approach
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Tsw
2
CrM operation is
maintained but
a perturbation of
the on-time may
degrade the
180° phase shift
General Principle on a Two-NCP1601 Solution
• The solution lies on the Frequency Clamp Critical
Conduction mode, unique scheme developed by ON
Semiconductor (NCP1601)
• Two NCP1601 drive two independent PFC branches:
– Auxiliary windings are used to detect the core reset of each branch
– The current sensing is shared by the two stages for protection only
(Over Current Limitation)
• The two branches are operating in voltage mode
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Synchronization: the Main Challenge
• One driver (DRV2) synchronizes the two branches so that:
– Branch 1 (DRV1) cannot turn high until a time τ has elapsed
– Branch 2 (DRV2) cannot dictate a new conduction phase within 2τ
• Hence:
– In fixed frequency operation, the switching period for each branch is
2τ and the two phases are naturally interleaved
– In CrM, the switching frequency is that imposed by the current cycle
(Tsw>2τ) and must stabilize out of phase.
• Possible slippages are contained by a phase compensation
circuitry (refer to www.onsemi.com for detailed AN available
in Q4 2008).
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NCP1601 Synchronization Capability
50 µA
OSC pin
+
100 µA
Cosc
5.0 V
/ 3.5 V
•
The oscillator
oscillates
between 3.5 and
5V
•
The NCP1601
generates a clock
when the
oscillator goes
below 3.5 V
•
The clock signal
is stored until
ZCD is detected
S
CLOCK
Q
Q
R
DRV
5V
Vosc
3.5 V
IL(coil
current)
Dead-time
ZCD
CLOCK
Fixed Frequency
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Critical Conduction Mode
Operation @ 230 Vrms, Medium Load
•
SYNC2
2τ
•
DRV2
SYNC1
•
•
τ
•
DRV1
Each stage operates
in fixed frequency
mode
Both branches are
synchronized to DRV2
A new DRV2 pulse
can take place after 2τ
A new DRV1 pulse
can occur after τ
The switching period
for each branch is
then 2τ and they
operate out of phase.
‰ A new drive sequence cannot take place as long as the SYNC signal remains
higher than 3.5 V (see NCP1601 operation).
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Operation at Low Line, Full Load
•
SYNC2
•
DRV2
•
SYNC1
•
DRV1
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The circuit operates in
critical conduction
mode
The operation of both
branches are
synchronized to DRV2
A new DRV2 pulse
can take place after
2τ, but the MOSFET
turn on is delayed until
the core is reset
A new DRV1 pulse
can occur after τ, but
again, the MOSFET
turn on is delayed until
the core is reset
Remarks on the Solution
•
•
•
The NCP1601 operates in voltage mode
Same on-time and hence switching period in the two branches
A coil imbalance
– Does not affect the switching period
– “Only” causes a difference in the power amount conveyed by each branch
Iin(1)
Iin(2)
L1 > L2
L
= 2
L1
Phase 1
Phase 2
ton
•
ton
time
The two branches are synchronized but they operate independently:
– Discontinuous conduction mode is guaranteed (zero current detection)
– No risk of CCM operation
– Both branches enter CrM at full load
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D16
1N5406
X5
LPRIM = 150u
LSEC = 1.5u
Application
Schematic
D5
MUR550
6
D15
1N4148
Vaux2
R17
2.2
22
16
Q2
2N2907
23
X6
SPP11N60
R20
10k
R21
47
EMI filter
X1
LPRIM = 150u
LSEC = 1.5u
U1
KBU6K
9
27
18
-
C8
100pF
Q1
2N2907
40
R2
1k
28
X4
SPP11N60
R11
10k
R31
820k
R16
47
14
D10
5V
The NCP1601
controllers are
fed by an
external 15 V
power source
C2x
100µF / 450V
R7
2.2
33
C10x
4.7nF
Type = Y1
Vbulk
11
D14
1N4148
C5
680nF
Type = X2
IN
D4
MUR550
24
+
C18
680nF
DRV2
R32
270k
45
D1
1N4148
15
R18
820k
C21
1nF
DRV1
CM1
R33
1k
C6
680nF
Type = X2
36
DRV1
C11
1.2nF
31
5
R22
75m / 3 W
7
13
3
6
19
4
5
26
7
R4
33k
R29
82k
Vfr
R14
820k
R27
270k
2
R8
1k
46
Vbulk
35
R5
820k
C13
1nF
D11
5V
R30
10
vcc
D6
1N4148
C19
100nF
C7
100nF
Vcontrol
54
R36
1k
R26
10k
R38
4.7k
R24
100
R19
3.9k
C1
1.2nF
12
C10
100µF /25 V
X3
NCP1601
4
DRV2
Vaux
8
1
2
7
29
3
6
44
4
5
DRV2
D3
1N4148
SYNC2
Circuitry for Frequency Foldback
R28
100k
R25
150k
vcc
DRV2
DRV1
R39
2.2k
34
C12
470pF
R12
2.2k
21
R35
2.2k
DRV1
R6
10k
DRV2
R9
10k
R15
10k
10
R40
2.2k
DRV2
25
Vfr
Circuitry for compensation of possible phase shift
C17
2.2nF
R10
100
8
C9
470pF
D2
1N4148
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D7
1N4148
SYNC1
C14
100pF
Earth
Wide mains,
300 W, PFC
pre-converter
DRV1
Circuitry for zero current detection
(branch 2)
Vaux2
90-265VAC
34
2
41
N
C20
100nF
8
1
C4
470pF
D12
1N5406
L
17
R23
100
Current sensing
X2
NCP1601
vcc
R37
3.9k
R1
3.9k
20
38
Vcontrol
R3
10k
Circuitry for zero
current detection
(branch 1)
39
L4
150µH
C2
100nF
1
C16
4.7nF
Type = Y1
Q3
2N2222
C3
10nF
D9
6.8V
R13
1k
The Board…
Wide mains,
300 W, PFC
pre-converter
MUR550
Two
NCP1601
circuits
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Buck
converter
to provide
Vcc (not
used for
test)
Input Voltage and Current
IL(tot) (2 A/div)
Vin (50 V/div)
Full load, 90 Vrms
IL(tot) (2 A/div)
Full load, 230 Vrms
Vin (100 V/div)
• As expected, the input current looks like a CCM one
• At high line, frequency foldback influences the ripple
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Zoom of the Precedent Plots
IL(tot) (2 A/div)
Full load, 90 Vrms
IL(tot) (1 A/div)
DRV1
Full load, 230 Vrms
DRV1
DRV2
DRV2
• These plots were obtained at the sinusoid top
• The current swings at twice the frequency of each phase
• At low and high line, the phase shift is substantially 180°
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No Overlap between the Refueling Sequences
Full load, 90 Vrms
IL(tot) (2 A/div)
IL(tot) (1 A/div)
Full load, 230 Vrms
Vds2
Vds1
Vds1
Vds2
• CrM at low line with valley switching
• Fixed frequency operation at high line (frequency foldback)
• No overlap between the demag. phases in both cases
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Performance Measurements
•
Conditions for the measurements:
– The measurements were made after the board was 30 mn operated full
load, low line
– All the measurements were made consecutively without interruption
– PF, THD, Iin(rms) were measured by a power meter PM1200
– Vin(rms) was measured directly at the input of the board by a HP 34401A
multimeter
– Vout was measured by a HP 34401A multimeter
– The input power was computed according to:
Pin ( avg ) = Vin ( rms ) ⋅ Iin ( rms ) ⋅ PF
– Open frame, ambient temperature, no fan
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Efficiency versus Load
100.0%
Results obtained
in a relatively
high frequency
application
allowing the use
of small
inductors:
(85 kHz in each
phase at 90 Vrms,
full load,
L1 = L2 =150 µH)
98.8%
Efficiency (%)
230 Vrms
97.5%
120 Vrms
96.3%
95.0%
90 Vrms
93.8%
92.5%
30
60
90
20% Pmax
120
150
180
210
240
270
Output power (W)
300
330
Pmax
‰ The plot portrays the efficiency over the line range, from 20% to 100% of the load
‰ The
efficiency remains higher than 95%!
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Switching Frequency (at the Sinusoid Top)
100.0
85 kHz
Switching frequency (kHz)
90.0
90 Vrms
80.0
70.0
60.0
120 Vrms
50.0
40.0
CrM lowers the
switching frequency
230 Vrms
30.0
Frequency foldback
20.0
30
60
90
120
150
180
210
240
270
300
330
Output power (W)
‰ The plot portrays fsw (sinusoid top) over the line range, as a function of the load
‰ The
PFC stages operate in CrM at full load
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Conclusion
• Interleaved PFCs
– Reduce the input current ripple
– Lower the bulk capacitor rms current
• Two NCP1601 provide an efficient solution for interleaving
• Besides interleaving, this solution takes benefit of:
– The FCCrM mode that optimizes the efficiency
– MUR550 diodes optimized for DCM PFC applications
– Frequency foldback (light load)
• The solution has been tested on a 300 W, wide mains board
• 95% efficiency at 90 Vrms over a large load range (from
20% to 100% load)
• A 16-pin interleaved PFC controller is under development
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Agenda
• Introduction
ƒ Basic solutions for power factor correction
ƒ New needs to address
• Interleaved PFC
ƒ Basic characteristics
ƒ A discrete solution
ƒ Performance
• Bridgeless PFC
ƒ
ƒ
ƒ
ƒ
Why should we care of the input bridge?
Main solutions
Ivo Barbi solution
Performance of a wide mains, 800 W application
• Conclusion
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No bridge!
The Diodes Bridge
Ac line
EMI
filter
+
+
PFC
stage
• The diodes bridge rectifies the ac line voltage
• Two diodes conduct simultaneously
• The PFC input current flows through two series diodes
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Efficiency Loss caused by the Diodes Bridge
• Average current flowing through the input diodes:
Ibridge
Tline
= Iline (t ) T
=
line
2 2
π
⋅
Pout
η ⋅Vin ( rms )
• Dissipation in the diodes bridge:
Pbridge = 2 ⋅Vf ⋅ Ibridge ≈ 2 ⋅Vf ⋅
• If Vf = 1 V and (Vin(rms))LL = 90 V:
2 2 ⋅ Pout
η ⋅ π ⋅Vin ( rms )
Pbridge ≈ 2% ⋅
Pout
η
Î In low mains applications (@ 90 Vrms), the diodes
bridge wastes about 2% efficiency!
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Basic Bridgeless PFC
Switching cell when PH2 is high
M1 is off
PH1
D1
D2
M1
M2
L
Ac Line
PH2
Switching cell when PH1 is high
M2 is off
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Operation with Positive Half-Wave
‰ PH1 is high, PH2 is low:
M1 is on: conduction time
M1 is open: off time
D1
PH1
Ac Line
M2
Body
diode
PH2
M1
‰ M2 body diode grounds PH2 as would a diode bridge.
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Operation with Negative Half-Wave
‰ PH1 is low, PH2 is high:
M2 is on: conduction time
M1 is open: off time
D2
PH1
Ac Line
PH2
M1
Body
diode
M2
‰ Both line terminals are pulsating at the switching frequency
‰ The pulsation swing is high (VOUT)
‰ HF noise that leads to a tedious EMI filtering
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Ivo Barbi Bridgeless Boost
PH1
Ac Line
« PH1 »
PFC
stage
« PH2 »
PFC
stage
PH2
DRV
Two PFC stages but:
– One driver with no need for detecting the active half-wave
– Improved thermal performance
– As with convential PFC stages, the negative phase is always
attached to ground. EMI issue is solved.
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Current Sharing
Phase 1 current (5 A/div)
0A
0A
Part of the active
phase current
flows throught the
inactive MOSFET
and coil!
Phase 2 current (5 A/div)
Part of the current flows…
… through the supposedly inactive MOSFET and coil
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Two Return Paths…
Small low frequency impedance
PH2 is the positive terminal
PH1
Ac Line
PH2
Body diode
0V
Vin
DRV
Rsense
MOSFET is on
MOSFET is off
Need for current sense transformers
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Schematic for 800 W Prototype
« PH1 » PFC stage
D7
CSD10060
L1
0.2m
X4
Diode bridge
PH1
2
PH1
+
C15
1µF
Type = X2
C16
1µF
Type = X2
IN
DRV1
RETURN
R12
15k
R18
10
D1
1N4007
C17
1µF
Type = X2
CM2
49
R14
390k
R13x
680k
R12x
680k
24
Vpin1
23
R1
2200k
C14
1 µF
Type = X2
30
C7
10nF / 63 V
D2x
1N4007
10
C18
4.7 nF
Type = Y2
C1
100nF / 63V
R23
680k
43
36
X5
NCP1653
C2
100nF
R6
100k
R22
680k
F1
10 A
39
CS
40
D3
1N5817
R5
390
1
NC
2
InA OutA 7
D8
CSD10060
L4
0.2m
22
NC 8
D4
1N4148
X7
CS
33
1
FB
Vcc 8
15 2
Vctrl
Drv 7
13 3
In
Gnd 6
CS
Vm 5
12 4
R4xx
2.2k
« PH2 » PFC stage
C28
220nF
PH2
53
R13
100
6
NCP1653
3
Gnd
4
InB OutB 5
Vcc 7
MC33152
Vcc2
DRV1
18
R20
15k
R17
10
R21
3R
32
C27
100pF
37
R21x
680k
C6
22µF
C24
220nF
C25
22µF
28
R3
470k
42
C13
1 µF
Type = X2
Vcc2
R15
10
Vcc1
C3
220nF
5
RETURN
51
R36
100
R2
2700k
X2
2*SPP20N60 (TO220)
R19
10k
Vout
R16
3R
31
9
R11
180k
Vaux
C5
10nF
27
CM1
CS
7
PH2
-
C19
4.7 nF
Type = Y2
D2
1N4148
X3
X1
2*SPP20N60 (TO220)
20
1
R7
56k
C4
1nF
R20x
10k
Vout
RETURN
3
R4x
2.2k
L
N
Earth
90 to 265 Vrms
50 or 60 Hz line voltage
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R4
33m
RETURN
C11
330u / 450 V
C12
330u / 450 V
Board Photograph
NCP1653
And
MC33152
MOSFET
driver
Bulk
converter to
generate the
Vcc voltage
(NCP1012)
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Typical Waveforms
Iline (10 A/div)
90 Vrms
230 Vrms
Iline (10 A/div)
Vout
Vout
CS (negative sensing)
CS (negative sensing)
Vin,1 (input voltage for branch 1)
Vin,1
•
•
•
These plots portray typical waveforms at full load (Iout = 2.1 A)
“CS” is representative of the current flowing into the MOSFETs of the
two branches (common output of the current transformers)
The input current is sinusoidal
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Zoom of the Precedent Plots
(Top of the Sinusoid)
90 Vrms
230 Vrms
Iline (10 A/div)
Iline (10 A/div)
Vout
Vout
Vin,1
Vsense (negative sensing)
Vin,1 (input voltage for branch 1)
•
•
The switching frequency is 100 kHz
The waveforms are similar to those of a traditional CCM PFC
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Vsense (negative sensing)
Performance Measurements
•
Conditions for the measurements:
– The measurements were made after the board was 30 mn operated full load,
low line
– All the measurements were made consecutively without interruption
– PF, THD, Iin(rms) were measured by a power meter PM1200
– Vin(rms) was measured directly at the input of the board by a HP 34401A
multimeter
– Vout was measured by a HP 34401A multimeter
– The input power was computed according to:
Pin ( avg ) = Vin ( rms ) ⋅ Iin ( rms ) ⋅ PF
– Open frame, ambient temperature, no fan
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Efficiency versus Load
100.0%
230 Vrms
Efficiency (%)
98.0%
120 Vrms
96.0%
90 Vrms
94.0%
92.0%
90.0%
100
200
20% Pmax
300
400
500
Output power (W)
600
700
800
Pmax
‰ The plot portrays the efficiency from 20% to 100% of the load
‰ At 90 Vrms, full load, it is about 94% without fan (95% at 100 Vrms)
‰ At 20% of full load, efficiency is in the range or higher than 96%
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THD versus Load
20.0
THD (%)
15.0
90 Vrms
10.0
230 Vrms
5.0
120 Vrms
0.0
100
200
20% Pmax
•
400
500
600
Output power (W)
THD remains very low on the whole range
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300
700
800
Pmax
900
Conclusion
• A bridgeless PFC controlled by the NCP1653 has been
developed (100 kHz)
• The prototype was tested at full load (800 W output) without
fan (open frame, ambient temperature)
• In these conditions, the efficiency was measured in the
range of 94% at 90 Vrms and 95% at 100 Vrms
• The THD remains very low
• Bridgeless can be an efficient solution for high power
applications.
• An application note is being prepared and should be posted
in Q4 this year.
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59
Agenda
• Introduction
ƒ Basic solutions for power factor correction
ƒ New needs to address
• Interleaved PFC
ƒ Basic characteristics
ƒ A discrete solution
ƒ Performance
• Bridgeless PFC
ƒ
ƒ
ƒ
ƒ
Why should we care of the input bridge?
Main solutions
Ivo Barbi solution
Performance of a wide mains, 800 W application
• Conclusion
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60
Conclusion
• New requirements:
• Compactness and form factor (LCD TV)
• Efficiency (ATX power supplies)
• New solutions can address them
• Interleaved PFC brings:
•
•
•
•
•
Efficiency
Flat design
Improved heat distribution
Reduced rms current through the PFC stage
Modular approach
• Bridgeless PFC:
• halves the losses in the input rectification
• Improves the heat distribution
• ON Semiconductor supports these innovative approaches
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61
For More Information
•
View the extensive portfolio of power management products from ON
Semiconductor at www.onsemi.com
•
View reference designs, design notes, and other material supporting
the design of highly efficient power supplies at
www.onsemi.com/powersupplies
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