Power Factor Correction using IR1152 Fixed Frequency CCM PFC IC

Application Note AN-1150
Power Factor Correction using
IR1152 Fixed Frequency CCM PFC IC
By Ramanan Natarajan, Helen Ding, Ron Brown
Table of Contents
IR1152 Detailed Description
PFC Converter Design Procedure using IR1152
PFC Converter Board Layout Tips
For additional data, please visit our website at:
http://www.irf.com
Keywords: PFC, Power Factor Correction, THD.
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1. Introduction
The IR1152 IC is a fixed 66kHz frequency PFC IC designed to operate in
continuous conduction mode Boost converters with average current mode
control. The IC is packed with an impressive array of advanced features such as
programmable soft-start, micro-power startup current, user initiated micro-power
Sleep mode for compliance with stand-by energy standards, ultra low bias
currents for sensing pins. The fixed internal oscillator ensures stable operation at
66kHz switching frequency with very low gate jitter thus eliminating audible noise
in PFC magnetics. In addition, the IC offers input-line sensed brown-out
protection (BOP), “dual & dedicated” overvoltage protection, cycle-by-cycle peak
current limit, open loop protection (OLP) and VCC under voltage lock-out
(UVLO). All these features are offered in a compact 8-pin package making
IR1152 the most feature-intensive IC for PFC applications. This application note
provides an overview of IR1152 and demonstrates the design of a universal input
350W AC-DC Boost PFC Converter. Design & layout tips are also included.
2. IR1152 – Detailed Description
2.1 Overview of IR1152
AC Line
Bridge
-
+
LBST
DBST
VOUT
AC Neutral
RVFB1
ROVP1
RVFB2
ROVP2
RVFB3
ROVP3
RBOP1
CIN
IR1152
IR1145
RBOP2
1
2
3
4
CBOP
CSF
COMP VCC
ISNS
VFB
BOPOVP/EN
8
7
6
RG
VCC
COUT
MBST
5
Rgm
RBOP3
RSF
COM GATE
CVCC
CP
CZ
COM
RSNS
GND
Fig.1: Typical application diagram of IR1152 based PFC converter
Fig.1 shows the system application diagram of the IR1152 based PFC converter.
Only 3 pin functionalities - VFB, COMP & ISNS – are actually needed to obtain
the necessary diagnostic signals to achieve power factor correction and maintain
output voltage regulation. The functions of the abovementioned 3 pins are as
follows:
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•
•
VFB – provides DC bus voltage sensing for voltage regulation
COMP – used for compensating the voltage feedback loop to set the correct
transient response characteristics
• ISNS – provides sensing of the inductor current, which is used to determine
the PFC switch duty cycle
Essentially, there are 2 control loops in the PFC algorithm:
• a slow, outer voltage loop whose function is to simply maintain output voltage
regulation
• a fast inner current loop whose function is to determine the instantaneous
duty cycle every switching cycle
The current shaping function i.e. power factor correction is achieved primarily by
the current loop. The voltage loop is responsible only for controlling the
magnitude of the input current in order to maintain DC bus voltage regulation.
2.2 Key Features of IR1152
Fixed 66kHz Frequency Internal Oscillator
IR1152 features a fixed frequency internal oscillator running at 66kHz. The gate
drive pulse is completely free of jitter and this greatly enables elimination of
audible noise in PFC magnetics due to magnetostriction. Also internalization of
the oscillator greatly improves noise immunity of the IC.
Programmable soft-start
IR1152 facilitates programmability of system soft-start time thus allowing the
designer enough freedom to choose the converter start-up times appropriate for
the application. The soft start time is the time required for the VCOMP voltage to
charge through its entire dynamic range i.e. 0V through VCOMP,EFF. As a result,
the soft-start time is dependent upon the component values selected for
compensation of the voltage loop on the COMP pin – primarily the CZ capacitor
(described in detail in Soft-Start Design section of PFC Converter Design portion
of this document). As VCOMP voltage rises gradually, the IC allows a higher and
higher RMS current into the PFC converter. This controlled increase of the input
current contributes to reducing system component stress during start-up. It is
clarified that, during soft-start, the IC is capable of full duty cycle modulation
(from 0% to MAX DUTY), based on the instantaneous ISNS signal from system
current sensing. Furthermore, the internal logic of the IC is designed to ensure
that the soft-start capacitor is discharged when the IC enters the Sleep or Standby modes in order to facilitate soft-start upon restart.
User initiated micro-power sleep mode
The IR1152 has an ENABLE function embedded in the OVP/EN pin. When this
pin voltage is actively pulled below VSLEEP threshold, the IC is pushed into the
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Sleep mode where the current consumption is less than 75uA even when VCC is
above VCC,ON threshold. The system designer can use an external logic level
signal to access the ENABLE feature since VSLEEP threshold is so low. The
IR1152 internal logic ensures that VCOMP is discharged before the IC enters Sleep
mode in order to enable soft-start upon resumption of operation.
Protection features
The IR1152 features a comprehensive array of protection features to safeguard
the system. These are explained below.
1. “Dual & Dedicated” Overvoltage protection (OVP)
Fig.2: IR1152 Overvoltage Protection Scheme (dual & dedicated)
There are 2 overvoltage comparators in IR1152 – the OVP(OVP) and OVP(VFB)
comparators. Both are identical in operation and also in terms of the overvoltage
trigger and release thresholds. The OVP(OVP) tracks the OVP/EN pin while the
OVP(VFB) tracks the VFB pin for output voltage information.
An overvoltage fault is triggered when either one or both of the pin voltage
exceeds the VOVP threshold of 106%VREF. The IC gate drive is immediately
disabled and held in that state. The overvoltage fault is removed and gate drive
re-enabled only when both pin voltages are below the VOVP,RST threshold of 103%
VREF. The tandem operation of the 2 comparators lends 2 important aspects to
the overvoltage protection feature in IR1152 that is not afforded by any
competitor, 8-pin PFC ICs:
• Dedicated OVP protection- The OVP pin is a dedicated pin for overvoltage
protection that safeguards the system even if there is a break in the VFB
feedback loop due to resistor divider failure etc.
• Dual OVP Protection- Each comparator acts as a watchdog for the other.
Under abnormal failure situations such as pin-to-pin shorts, if for any reason
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one of the comparator misbehaves, the other comparator still provides
overvoltage protection.
Since the VFB pin which programs the DC bus regulation voltage through the
voltage error amplifier also features an overvoltage comparator with 106%VREF
threshold, this effectively fixes the system maximum overvoltage protection level
at 106% of the nominal regulation voltage level. Though a lower level of
overvoltage protection can be set through the dedicated OVP pin, care must be
taken to avoid setting the protection threshold too low. A lower overvoltage
protection threshold could cause the OVP reset threshold lower than 100% of the
nominal output voltage, which may trigger multi OVP protections during startup.
Thus it is recommended to set the overvoltage protection threshold to the default
106%VREF. In another word, the voltage divider that connected to OVP pin should
use the same value as the VFB voltage divider.
2. Open-Loop protection (OLP)
The open-loop protection ensures that the IC is restrained in the Stand-by mode
if the VFB pin voltage has not exceeded or has dropped below VOLP threshold of
19%VREF. In the Stand-by mode, all internal circuitry of the IC are biased, the
gate drive is disabled and current consumption is a few milliamps. During startup, if for some reason the voltage feedback loop is open then IC will remain in
Stand-by and not start thus avoiding a potentially catastrophic failure.
3. Brown-Out protection (BOP)
IR1152 provides brown-out protection based on direct sensing of AC input line.
Information about the rectified AC input voltage is communicated to the BOP pin
after scaling it down using a resistor divider network and filtering using a
capacitor on BOP pin. During start-up, the IC is held in Stand-by mode when
BOP pin voltage is less than VBOP(EN) threshold of 1.56V. When the pin voltage
exceeds this threshold, the IC enters normal operation (assuming no OLP
condition exists). Subsequently, if the pin voltage falls below VBOP threshold of
0.76V during normal operation, then a brown-out fault is detected and IC is
pushed into Stand-by mode. For the IC to exit Stand-by, the pin voltage has to
exceed VBOP(EN) threshold again. In the Stand-by mode, all internal circuitry of the
IC are biased, the gate drive is disabled and current consumption is a few
milliamps.
4. Cycle-by-cycle peak current limit protection (IPK LIMIT)
The cycle-by-cycle peak current limit is encountered when VISNS pin voltage
exceeds VISNS(PK) threshold of -0.75V (in magnitude). When this condition is
encountered, the IC gate drive is immediately disabled and held in that state until
the ISNS pin voltage falls below VISNS(PK). Even though the IR1152 operates
based on average current mode control, the input to the peak current limit
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comparator is decoupled from the averaging circuit thus enabling instantaneous
cycle-by-cycle protection for peak current limitation.
5. VCC UVLO
In the event that the voltage at the VCC pin should drop below that of the VCC
UVLO turn-off threshold, VCC(UVLO) the IC is pushed into the UVLO mode, the gate
drive is terminated, and the turn on threshold, VCC, ON must again be exceeded in
order to re start the process. In the UVLO mode, the current consumption is less
than 75uA.
3. PFC Converter Design Procedure
3.1 PFC Converter Specifications
AC Input Voltage Range
85-264VAC
Input Line Frequency
47-63Hz
Nominal DC Output Voltage
385V
Maximum Output Power
350W
Power Factor
0.99 @ 115VAC/350W
0.99 @ 230VAC/350W
Minimum Output Holdup Time
25ms @ VOUT,MIN=285V
Maximum Soft Start Time
60msec
Table 1: Design Specifications for PFC Converter
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3.2 Power Circuit Design
AC Line
Bridge
-
+
LBST
DBST
VOUT
AC Neutral
RVFB1
ROVP1
RVFB2
ROVP2
RVFB3
ROVP3
RBOP1
CIN
IR1152
IR1145
RBOP2
1
2
3
4
CBOP
CSF
COMP VCC
ISNS
VFB
BOPOVP/EN
8
7
6
RG
VCC
COUT
MBST
5
Rgm
RBOP3
RSF
COM GATE
CVCC
CP
CZ
COM
GND
RSNS
Fig.3: IR1152 based PFC Boost Converter
Peak Input Current
It is necessary to determine the maximum input currents (RMS & peak) from the
specifications in Table 1 before proceeding with detailed design of the PFC boost
converter. The maximum input current is typically encountered at highest load &
lowest input line situation (350W, 85VAC). Assuming a nominal efficiency of 92%
at this situation, the maximum input power can be calculated:
PIN ( MAX ) =
PO ( MAX )
η MIN
=
350W
= 380W
0.92
From this, the maximum RMS AC line current is then calculated:
I IN ( RMS ) MAX =
I IN ( RMS ) MAX =
PO ( MAX )
η MIN (V IN ( RMS ) MIN ) PF
350W
= 4.5 A
0.92(85V )0.998
The selection of the semiconductor components (bridge rectifier, boost switch &
boost diode) is based on IIN(RMS)MAX =4.5A.
Assuming a pure sinusoidal input, the maximum peak AC line current can then
be calculated:
I IN ( PK ) MAX =
I IN ( PK ) MAX =
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2 ( PIN ( MAX ) )
V IN ( RMS ) MIN
1.414(380W )
= 6. 3 A
85V
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Boost Inductance (LBST)
IR1152 IC is an average current mode controller. An on-chip RC filter is sized to
effectively filter the boost inductor current ripple to generate a clean average
current signal for the IC. The averaging function in the IC can accommodate a
maximum limit of 40% inductor current ripple factor at maximum input current.
The boost inductance has to be sized so that the inductor ripple current factor is
not more than 40% at maximum input current condition (at peak of AC sinusoid).
This is because:
• Higher ripple current factors will interfere with the Average Current Mode
operation of One Cycle Control algorithm in IR1152 leading to duty cycle
instabilities and pulse skipping which results in current distortion and
sometimes even audible noise
• power devices are stressed more with higher ripple currents as the peak
inductor current (IL(PK)MAX) also increases proportionately
In this calculation, an inductor current ripple factor of 35% is selected (typical
ripple factor is ~20% for most PFC designs). The ripple current at peak of AC
sinusoid at maximum input current is:
∆I L = 0.35 × I IN ( PK ) MAX
∆I L = 0.35 × 6.3 A = 2.2 A
And, peak inductor current is:
I L ( PK ) MAX = I IN ( PK ) MAX +
∆I L
2
2.2 A
2
= 7.4 A
I L ( PK ) MAX = 6.3 A +
I L ( PK ) MAX
In order to determine the boost inductance, the power switch duty cycle at peak
of AC sinusoid (at lowest input line of 85VAC) is required.
VIN ( PK ) MIN = 2 × VIN ( RMS )MIN = 120V
Based on the boost converter voltage conversion ratio,
D=
D=
VO
VIN ( PK ) MIN
VO
385V − 120V
= 0.69
385V
The boost inductance is then given by:
L BST =
V IN ( PEAK ) MIN × D
f SW × ∆I L
=
120V × 0.69
66kHz × 2.2 A
L BST = 570µH
A convenient value of 600µH is selected for LBST for this converter which will
result in an inductor ripple current factor between 30-35%.
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High Frequency Input Capacitor (CIN)
The purpose of the high-frequency capacitor is to supply the high-frequency
component of the inductor current (the ripple component) via the shortest
possible loop. This has the advantage of acting like an EMI filter, since it
minimizes the high-frequency current requirement from the AC line. Typically a
high-frequency, film type capacitor with low ESL and high-voltage rating (630V) is
used.
High-frequency input capacitor design is essentially a trade-off between:
• sizing it big enough to minimize the noise injected back into the AC line
• sizing it small enough to avoid line current zero-crossing distortion (flattening)
The high-frequency input capacitor is determined as follows:
C IN = k ∆I L
I IN ( RMS ) MAX
2π × f SW × r × VIN ( RMS ) MIN
4.5 A
2π × 66kHz × 0.09 × 85V
= 0.496µF
C IN = 0.35
C IN
where:
k∆IL = inductor current ripple factor, of 35% as mentioned earlier
r = maximum high frequency input voltage ripple factor (∆VIN/VIN), assumed 9%
A standard 0.470µF, 630V capacitor is selected for CIN for this converter.
Output Capacitor (COUT)
Output Capacitor design is based on hold-up time requirement
For 25ms hold-up time and minimum output voltage of 285V the output
capacitance is first calculated:
2 ⋅ P ⋅ ∆t
C OUT ( MIN ) = 2 O
2
VO − VO ( MIN )
2 ⋅ 350W ⋅ 25ms
(385V ) 2 − (285V ) 2
COUT ( MIN ) = 261µF
C OUT ( MIN ) =
Minimum capacitor value must be de-rated for capacitor tolerance (20%) to
guarantee minimum hold-up time.
COUT ( MIN ) 261µF
COUT =
=
= 326µF
1 − ∆CTOL 1 − 0.2
A standard 330µF, 450V capacitor is selected for COUT for this converter.
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3.3 IR1152 Control Circuit Design
3.3.1 Current Sense Resistor Design (ISNS pin)
In IR1152, there are two levels of current limitation:
- a “soft” current limit, which limits the duty-cycle and causes the DC bus
voltage to fold-back i.e. droop
- a cycle-by-cycle “peak” current limit feature which immediately terminates
gate drive pulse once the ISNS pin voltage exceeds VISNS,PEAK
“Soft” Current Limit
In IR1152 the COMP pin voltage is directly proportional to the RMS input current
into the PFC converter i.e. VCOMP is higher at higher RMS current. Clearly its
magnitude is highest at maximum load PMAX & minimum AC input voltage, VIN,MIN.
The dynamic range of VCOMP in the IC is defined by VCOMP,EFF parameter in the
IR1152 datasheet. Once VCOMP signal saturated (reaches VCOMP,EFF), any system
requirement causing an additional increase in current will cause the IC to
respond by limiting the duty cycle and thereby causing the output voltage to
droop. This is called “soft” current limit protection. The selection of RSNS must
ensure that “soft” current limit is not encountered at any of the allowable line and
load conditions.
RSNS Design
The design of RSNS is performed at the system condition when the inductor
current is highest at lowest input line (VIN,MIN) and highest load (PMAX). Further,
the inductor current is highest at the peak of the AC sinusoid. The duty cycle
required at peak of AC sinusoid at VIN,MIN=85VAC in order to regulate VOUT=385V
is:
DPEAK =
DPEAK =
VOUT − 2V IN ( RMS ) MIN
VOUT
385V − 2 .85V
= 0.69
385V
RSNS design should guarantee that
i. PFC algorithm can deliver this duty cycle at peak of AC sinusoid at VIN,MIN &
PMAX condition
ii. soft current limit is encountered whenever there is a further increase in
demand for current while operating at VIN,MIN & PMAX condition
To do this, the VISNS is calculated below.
V ISNS ( MAX ) =
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VCOMP ( EFF )( MIN ) ⋅ (1 − D )
g DC
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V ISNS ( MAX ) =
4.7V ⋅ (1 − 0.69 )
= 0.47V
3 .1
Note: if the calculated VISNS(MAX) is higher than the cycle-by-cycle peak
overcurrent limit specification of the IC, the VISNS(PK) value should be used to
determine RSNS. In this example, VISNS(MAX) is lower than 0.68V VISNS(PK)(MIN) thus
0.47V is used for RSNS calculation.
Next the peak inductor current at maximum peak AC line current, derated with an
overload factor (KOVL=10%), is calculated.
I IN ( PK )OVL = I L ( PK ) max .(1 + K OVL )
I IN ( PK ) OVL = 7.4 × 1.1 = 8.2 A
From this maximum current level and the required voltage on the current sense
pin, we now calculate the maximum resistor value that can be used for the PFC
converter.
RSNS ,MAX =
VSNS (max)
I IN ( PK ) OVL
=
0.47V
8.2 A
RSNS ,MAX = 0.057Ω
It is noted that even though IR1152 operates in average current mode it is still
safer to use the peak inductor current for current sense resistor design to
guarantee avoiding premature fold-back.
Power dissipation in the resistor is now calculated based on worst case RMS
input current at minimum input voltage:
PRS = I IN ( RMS )MAX ⋅ RS
2
PRS = 4.5 2 (0.057Ω) = 1.2W
A standard 50mΩ resistor can be selected for RSNS for the PFC converter.
Peak Current Limit
The cycle-by-cycle peak current limit is encountered when VISNS pin voltage
exceeds VISNS,PEAK. For the PFC converter, this limit is encountered whenever the
inductor current exceeds the following:
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I PK _ LMT =
− .75V
= 15 A
0.05Ω
It is clarified that even though the IR1152 operates based on average current
mode control, the input to the peak current limit comparator is decoupled from
the averaging circuit thus enabling instantaneous cycle-by-cycle protection for
peak overcurrent.
IR1152
IR1145
RBOP2
1
2
3
4
CBOP
CSF
COMP VCC
ISNS
VFB
BOPOVP/EN
R
8
7
V
6
5
Rgm
RBOP3
RSF
COM GATE
CVCC
CP
CZ
COM
GND
RSNS
Fig 4: Current Sense Resistor and Filtering
The current sense signal is communicated to the ISNS pin of the IC using a
current limiting series resistor, RSF. An external RC filtering for ISNS pin can be
realized (though not necessary for IR1152) by adding a filter capacitor, CSF
between the ISNS pin and COM as shown in Fig.4. A corner frequency around 11.5MHz will offer a safe compromise in terms of filtering, while maintaining the
integrity of the current sense signal for cycle-by-cycle peak overcurrent
protection.
1
f PSF =
2π ⋅ RSF ⋅ C SF
With RSF=100Ω, we can use CSF=1000pF to obtain a cross-over frequency of
1.6MHz. The input impedance of the current sense amplifier is approximately
25KΩ. The RSF resistor will form a divider with this 25KΩ resistor. For RSF=100Ω
it is noted that the accuracy of the current sense voltage signal communicated to
the IC is more than 99.5%.
3.3.2 Output Regulation Voltage Divider (VFB pin)
The output regulation voltage of the PFC converter is set by voltage divider on
VFB pin - RFB1, RFB2, and RFB3. The total impedance of this divider network must
be high enough to reduce power dissipation, but low enough to keep the
feedback voltage error (due to finite bias currents into the voltage error amplifier
which is less than 0.2uA) negligible. Around 2MΩ is an acceptable value for the
total resistor divider impedance.
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A standard 1MΩ, 1% tolerance resistor is selected for RFB1 & RFB2 for this
converter. Then, RFB3 is determined based on error amplifier VREF (Typ)=5V and
VOUT=385V converter specification.
R FB 3 =
RFB 3 =
V REF ( R FB1 + R FB 2 )
(Vout V REF )
5.0V ( 2000k )
= 26.3kΩ
(385V - 5.0V )
A standard resistor, RFB3 = 26.1kΩ, 1% tolerance, is selected for this converter.
The new regulation VOUT value based on actual resistor values is then calculated.
VOUT =
VOUT =
( RFB1 + RFB 2 + RFB 3 ) ⋅ VREF
RFB 3
( 2000k + 26.1k) ⋅ 5.0V
= 388.1V
26.1k
Power dissipation of divider resistors is given by the following.
PRFB1 = PRFB 2 =
PR FB 1 = PR FB 2 =
(Vout − VREF )2
2(RFB1 + RFB 2 )
(388.1V − 5V )2
4 × 1000k
= 37mW
VFB is a multi-function pin with the following functionalities:
•
The VFB pin is an input to the open-loop comparator that references a VOLP
threshold of 19% of VREF. The IC is restrained in the Stand-by Mode
whenever VFB pin is less than VOLP.
•
The VFB pin is also non-inverting input to the overvoltage comparator. This
comparator is designated the OVP(VFB) comparator in the IC Block diagram
in the datasheet. The typical overvoltage set-point is VOVP=106%VREF and the
re-enable set-point is VOVP(RST)=103%VREF.
VOVP = 1.06 ⋅V REF = 5.30V
VOVP ( RST ) = 1.03 ⋅ V REF = 5.15V
Using the resister divider determined earlier, it is a straightforward calculation
to obtain the overvoltage trigger/re-enable set-points.
V OVP = 1 .06 ⋅ VOut
V OVP = 1 .06 × 388 .1 = 412V
V OVP ( RST ) = 1 . 03 ⋅ V Out
V OVP ( RST ) = 1 . 03 × 388 . 1 = 400 V
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3.3.3 Dedicated Overvoltage Protection Divider (OVP/EN pin)
In addition to the overvoltage comparator on VFB pin, IR1152 features a 2nd
overvoltage comparator (designated the OVP(OVP) in the IC block diagram)
which is connected to the OVP/EN pin. The OVP(OVP) comparator is identical in
design to the OVP(VFB) comparator and also references the same trigger and
re-enable thresholds of 106% and 103% of VREF respectively. The VFB pin
resistor divider calculated earlier is applicable for the OVP/EN pin also. Hence,
for this converter, 1Mohm, 1% tolerance resistor is selected for ROVP1 & ROVP2
and 26.1kΩ, 1% tolerance resistor is selected for ROVP3. The trigger and reenable set-points calculated earlier are likewise applicable here too.
3.3.4 Brown-Out Protection R/C Circuit (BOP pin)
IR1152 provides brown-out protection based on direct sensing of rectified AC
input line. Information about the rectified AC input voltage is communicated to the
BOP pin after scaling it down using a resistor divider network and filtering using a
capacitor on BOP pin as shown below. This R/C network is essentially a voltagedivision/averaging network. The sinusoidally varying rectified AC voltage is
divided by the resistor divider and averaged by the capacitor and presented at
the BOP pin as a DC level, VBOP, AVG along with some ripple, ∆VBOP. The BOP pin
R/C circuit is illustrated in Fig.5. The BOP pin voltage is illustrated in Fig.6.
Bridge
+
LBST
RBOP1
CIN
IR1152
IR1145
RBOP2
1
2
3
4
ISNS
VFB
BOPOVP/EN
8
7
6
5
C
CBOP
CSF
COMP VCC
Rgm
RBOP3
RSF
COM GATE
CP
CZ
COM
GND
RSNS
Fig 5: Brown-out protection circuit for IR1152
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900mV
∆VBOP
VBOP
VBOP,AVG
750mV
SEL>>
600mV
V(R2:2)
80V
VIN
40V
0V
1/2fAC
Fig 6: Voltage waveform on the BOP pin is comprises a DC level (VBOP,AVG) and a
ripple voltage (∆VBOP)
The DC level VBOP,AVG is given by:
V BOP , AVG =
R BOP 3
⋅ V ACAVG
RTOT
where
RTOT = RBOP1+RBOP2+RBOP3
V AC , AVG =
2
π
2 ⋅ V IN ( RMS )
Hence:
V BOP , AVG =
R BOP 3 2
⋅
2 ⋅ V IN ( RMS )
RTOT π
Thus VBOP,AVG depends only on the resistor divider and the AC input voltage.
The ripple ∆VBOP is given by the transfer function represented by the resistor
divider and the capacitor:
T (s) =
∆V BOP R BOP 3
=
⋅
V AC , PK
RTOT
1
1 + sC BOP ⋅
( R BOP1 + R BOP 2 ) R BOP 3
RTOT
Thus:
∆V BOP = 2 ⋅ V IN ( RMS ) ⋅
R BOP 3
⋅
RTOT
1
1+ (
ω 2
)
ωO
where:
ω = 2π ⋅ (2 ⋅ f AC )
ωO =
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( R BOP1
RTOT
+ R BOP 2 ) ⋅ R BOP 3 ⋅ C BOP
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∆VBOP magnitude is related to CBOP – bigger the capacitor, smaller the ripple.
During start-up, the IC is held in Stand-by mode when the BOP pin voltage, VBOP
is less than VBOP(EN)=1.56V. Next, when the AC voltage is applied and the BOP
pin voltage exceeds this threshold, the IC enters normal operation (assuming all
other conditions for normal operation are satisfied). If it is assumed that the
system is starting under no load, then the rectified AC voltage is essentially a DC
voltage and the BOP pin voltage is also DC.
V BOP =
R BOP 3
R
⋅ V AC , PK = BOP 3 ⋅ 2 ⋅ V IN ( RMS )
RTOT
RTOT
Under this condition, the AC voltage at which the IC becomes operational is
given by:
RBOP 3
⋅ 2 ⋅ VIN ,ON ( RMS ) > 1.56V
RTOT
However, if the system is starting up under a loaded condition, then the rectified
AC voltage is a varying sinusoidal function. In this case, the BOP pin voltage is
as described before (DC level + superimposed ripple). In this case, the IC
becomes operational when the maxima of VBOP exceeds VBOP(EN)=1.56V.
VBOP,MAX = VBOP,AVG + ∆VBOP /2 > 1.56V
Hence the exact AC voltage at which the IC becomes operational depends on
the load condition at start-up. CBOP must be big enough to ensure that ∆VBOP is
greater than the BOP hysteresis (1.56-0.76=0.8V) at the required minimum AC
input voltage, should the system start-up under a loaded condition.
Once the IC becomes operational and starts boosting the DC voltage, then the
rectified AC voltage will show sinusoidal variation. Subsequently, if the AC
voltage is reduced then VBOP,AVG & ∆VBOP both decrease in magnitude. When the
minima of the BOP pin voltage encounters the Brown-out trip threshold
VBOP=0.76V then the IC enters brown-out fault mode.
VBOP,MIN = VBOP,AVG - ∆VBOP /2
When a Brown-out fault is encountered, the gate pulse is immediately
terminated, the COMP pin is actively discharged, ICC current consumption falls
to a few milli-amperes and the BOP pin voltage has to exceed VBOP,EN once again
for the IC to restart.
The condition at which IC enters Brown-Out fault is then given by:
VBOP,MIN < 0.76V
The high input impedance and low bias current (<1uA) of the BOP comparator
allows a high impedance to be used for the BOP divider network. 5-10MΩ is an
acceptable range. A standard 3MΩ, 1% tolerance resistor is selected for RBOP1 &
RBOP2 for this converter. RBOP3 is selected based on VAC,ON, the AC input voltage
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AN-1150
16
at which the converter is expected to start-up. Assuming VAC,ON=65VAC and noload condition at start-up,
RBOP 3 =
V BOP ( HI ) ( R BOP1 + R BOP 2 )
( 2.V AC ,ON
1.56V (3MΩ + 3MΩ)
RBOP 3 =
RBOP 3
VBOP ( HI ) − V Bridge )
( 2. 65VAC − 1.56V - 2V)
= 105.9kΩ
Next, assuming a target VAC,OFF=55VAC, CBOP has to be selected. First VBOP,AVG
is calculated at VAC,OFF:
V BOP , AVG =
V BOP , AVG =
2.V AC ,OFF ( R BOP 3 )
(π / 2).( R BOP1 + R BOP 2 + R BOP 3 )
2.55V AC .105.9kΩ
(π / 2).(3MΩ + 3MΩ + 105.9kΩ)
V BOP , AVG = 0.86V
Then, forcing VBOP,MIN (=VBOP,AVG - ∆VBOP/2) = 0.76V, we can calculate the
required ∆VBOP at VAC,OFF. At VAC,OFF=55VAC, this yields
∆VBOP = 2*(0.86-0.76) = 0.2V
In order to calculate CBOP, we just have to force the magnitude of the transferfunction at f=2*fAC=126Hz to be equal to 0.2V calculated above (maximum fAC is
the design condition that needs to be considered to ensure that the IC is
guaranteed to terminate operation at VAC,OFF. At a lower fAC, when there is higher
ripple, the IC will cease operation at a higher VAC). Thus:
∆V BOP = 2 ⋅ V AC ,OFF ⋅
R BOP 3
⋅
RTOT
1
ω
1 + ( )2
ωO
= 0.2V
where:
ω = 2π ⋅ (2 ⋅ f AC )
ωO =
1
1+ (
ω 2
)
ωO
= 0.2V ×
( R BOP1
RTOT
+ R BOP 2 ) ⋅ R BOP 3 ⋅ C BOP
RTOT
1
6.1059MΩ
1
×
= 0.2V ×
×
= 0.148
RBOP3
0.1059MΩ
2 ⋅V AC ,OFF
2 ⋅ 55Vac
ω = 2π ⋅ (2 ⋅ f AC ) = 2π ⋅ (2 ⋅ 63) = 791.68
ωo is then calculated to be:
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AN-1150
17
ωo = 118
From ωo, CBOP is calculated:
C BOP =
RTOT
6.1059MΩ
=
= 81nF
( R BOP1 + R BOP 2 ) ⋅ R BOP 3 ⋅ ω O 6 MΩ × 0.1059 MΩ × 118
For the converter, we can choose the following:
RBOP1 = RBOP2 = 3Mohm
RBOP3 = 100kohm
CBOP=100nF
Since selected RBOP3 is slightly less than what was calculated, VAC,ON will be
slightly higher than 65VAC. Since selected CBOP is slightly higher than what was
calculated, VAC,OFF will be slightly lower than 55VAC.
3.3.5 Voltage Loop Compensation (COMP pin)
The voltage feedback loop monitors the DC bus voltage (VOUT) via the VFB
resistor divider whose transfer function is H1(s). Comparison of the VFB pin
voltage and internal reference voltage of the IC by voltage error amplifier yields a
control signal (Vm = VCOMP-VCOMP,START). The transfer function of the error
amplifier and compensation network is H2(s). The IR1152 output voltage error
amplifier is a trans-conductance type amplifier and output of the error amplifier is
connected to the COMP pin. The control signal directly controls the magnitude of
the boost inductor current (IL), which is also the input current of the PFC
converter. The transfer function between IL and control signal Vm is given by
H3(s). The power stage of the PFC converter along with DC bus capacitor,
maintains a constant voltage (VOUT) at the converter output where the system
load draws energy from the converter. The power stage + DC bus capacitor +
system load transfer function is given by G(s). The small-signal model of the
voltage feedback loop is depicted below in Fig.7. The overall loop gain transfer
function T(s) is given by:
T(s) = H1(s).H2(s).H3(s).G(s)
vIN
∆
+
vREF
_
vFB
Error Amplifier +
Compensator
H2(s)
vm
OCC PFC
Modulator
H3(s)
iL
Plant
G(s)
vOUT
Output Divider
H1(s)
Fig.7: Small-signal modeling of the PFC voltage feedback loop
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AN-1150
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Voltage loop compensation is performed by adding R/C components between
COMP and COM pins in order to:
i.
Achieve the appropriate dynamic response characteristics during load/line
fluctuations
ii.
Ensure that the 2*fAC ripple in VOUT at steady state conditions, does not
cause too much current distortion
In order to evaluate the overall loop gain transfer function T(s), the small-signal
transfer function of each of the blocks has to be evaluated first.
Plant Gain, G(s)
The plant gain G(s) models the small signal variation in the DC bus voltage when
a small perturbation occurs in the boost inductor current.
G(s) = vOUT/iL = (vOUT/iCHG).(iCHG/iL)
where the small signal parameters are italicized and iL is the boost inductor
current, vOUT is the bus voltage and iCHG is the current sourced at the output of
the boost converter power stage (i.e. boost diode current).
+
COUT
SYSTEM
LOAD
VOUT/IOUT
(VIN/kM).. vm
(2MIOUT/VOUT).. vi
ichg
vOUT
RL
_
Fig.8: Small-signal model of PFC converter power stage
If the system load is a Resistive Load, the transfer function is:
v out
RL / 2
=
R
i chg
1 + sC out L
2
In the power stage transfer function, this is represented by a pole:
1
f PS =
R
2π ⋅ C out L
2
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AN-1150
19
For a Constant Power Load, the shunt impedance and the system load cancel
each other out and the equivalent impedance is infinite, in which case the
transfer function reduces to:
vout
1
=
ichg sCout
In the power stage transfer function, this is represented by a pole at the origin.
Under a Constant Current Load, since the impedance of a current source is
infinitely high, the equivalent impedance is effectively just the shunt impedance:
v out
RL
=
i chg 1 + sC out RL
In the power stage transfer function, this is represented by a pole:
1
f PS =
2π ⋅ C out R L
Next (iCHG/iL) transfer function has to be evaluated. Assuming 100% efficiency,
recognize that:
VIN.IL = VOUTIOUT
IOUT is same as the DC component of the boost diode current (ICHG). Hence
VIN.IL = VOUTICHG
Applying linearization and small-signal analysis, for a given DC operating point
defined by VIN & VOUT yields the relationship between iCHG & iL:
iCHG/iL = VIN/VOUT
Assuming a resistive load, the overall power stage transfer function can now be
written as:
RL / 2
VIN
G (s) =
×
R
VOUT
1 + sC out L
2
OCC PFC Modulator, H3(s)
In order to derive iL/vm, the One Cycle Control PWM modulator control law is
employed:
G DC ⋅ R S ⋅ i L =
vm
M (d )
where M(d) = VOUT/VIN for a given DC operating point defined by the DC bus
voltage VOUT and RMS input voltage VIN. This ultimately yields
H 3 (s) =
www.irf.com
iL
Vin
=
v m VOUT R S G DC
AN-1150
20
Output voltage sensor Resistor-Divider, H1(s)
The output divider scales the output voltage to be compared with the reference
voltage in the error amplifier.
Therefore:
VOUT =
( RFB1 + RFB 2 + RFB 3 )VREF
RFB 3
H 1 ( s) =
V REF
VOUT
The uncompensated loop gain and phase is shown in Fig.9 for 85-264VAC at
350W load condition (assuming resistive load). This is simply the H1(s).H3(s).G(s)
transfer function product illustrating the pole due to the plant gain.
90
90
Gain 85VAC Uncompensated
60
60
Gain 264VAC Uncompensated
Phase 85VAC Uncompensated
30
30
Phase 264VAC Uncompensated
0
-30
-30
-60
-60
-90
-90
-120
-120
-150
-150
-180
0.01
0.1
1
10
100
1000
10000
Phase (deg)
Gain (dB)
0
-180
100000
f (Hz)
Fig.9 The uncompensated transfer function [=H1(s).H3(s).G(s)]
Error Amplifier & Compensation, H2(S)
The compensation scheme typically employed for a first-order, single-pole
system aims to:
• add a pole at the origin in order to increase the low frequency gain and
improve DC regulation
• add a low-frequency zero to boost phase margin near cross-over frequency
and partially compensate the pole
• add a high-frequency pole to attenuate switching frequency noise and ripple
effects
The above 3 requirements can be achieved in case of the transconductance type
voltage error amplifier with the compensation scheme shown in Fig.10. However,
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AN-1150
21
as mentioned earlier, for the PFC converter, the most important criterion for
basing the selection of the compensation component values is the voltage loop
bandwidth.
Fig10: Voltage Loop error amplifier compensation network
The error amplifier transfer function is given by:
H 2( s ) =
g m ⋅ ( 1 + sRgmCZ )
s( C Z + C P + sRgmC Z C P )
where gm is the transconductance of the voltage error amplifier. The
compensation network adds a zero and a pole in the transfer function at:
fZ0 =
f P0 =
1
2π ⋅ Rgm ⋅ C Z
1
Cz ⋅ Cp
2π ⋅ Rgm
Cz + Cp
The gain and phase of the error amplifier + compensation transfer function is
illustrated in Fig.11.
90
90
EA Gain
EA Phase
60
30
30
0
0
-30
-30
-60
-60
-90
-90
-120
-120
-150
-150
-180
0.01
0.1
1
10
100
1000
10000
Phase (deg)
Gain (dB)
60
-180
100000
f (Hz)
Fig.11: Error Amplifier + compensation transfer function characteristics
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AN-1150
22
Voltage Loop Compensation procedure
Step 1: Choose Cz based on soft-start time:
A soft-start time of 60ms is selected. Typical values range from 50ms to a few
hundred ms, depending upon the application. The soft-start time represents the
time needed by the controller to ramp VCOMP from zero to the maximum value.
The system will take no more than 60ms to achieve near-regulation.
CZ =
t SS ⋅ iOVEA
V
COMP ( EFF )
( MIN )
iOVEA and VCOMP(EFF)(MIN) are taken from the datasheet.
CZ =
60ms × 44 µA
= 0.56 µF
4.7V
A standard value of 0.56uF can be selected for the converter for CZ.
Step 2: Choose Rgm to ensure that H1(s).H2(s) attenuation at 2xfAC frequency is
small enough to avoid current distortion:
The amount of 2xfAC ripple on the output capacitor is calculated first. The
minimum fAC of 47Hz is considered here, since the ripple is the maximum at the
lowest AC frequency. The peak-to-zero ripple VOPK is given by:
VOPK =
Pin , MAX
2π ⋅ 2 ⋅ f AC ⋅ C O ⋅ Vout
380W
2π ⋅ 2 ⋅ 47 ⋅ 330µF ⋅ 385V
= 5.1V
VOPK =
VOPK
The peak-to-peak ripple in VOUT is 2xVOPK. This ripple in VOUT is reflected in the
VCOMP voltage based on the attenuation provided by the resistor divider and error
amplifier compensation network combined i.e. H1(s).H2(s) at 2xfAC. The ripple in
VCOMP i.e. ∆VCOMP has to be small compared with the value of the error amplifier
output voltage swing (VCOMP,EFF). Typical values for ∆VCOMP/VCOMP range from
0.5% to 1%. 0.5% is recommended if current shaping has to be excellent while
1% is recommended for higher phase margin and low-oscillation response to
load steps. 0.5% attenuation demands a (GVA) of:
GVA =
www.irf.com
VCOMP ( EFF ) ⋅ 0.005
2 ⋅ VOPK
AN-1150
23
4.7V ⋅ 0.005
= 0.0023
2 ⋅ 5.1V
= −52.7 dB
GVA =
GVA
This is the required attenuation in H1(s).H2(s) at 2xfAC frequency.
H1(s), given by VREF/VOUT, is next calculated:
5V
H1 =
= 0.013 = −37.7dB
385V
The required attenuation from H2(s) alone at 2x47Hz is then given by:
GVA − H 1 = −15dB
Since the error amplifier pole will be set at a much higher frequency than 2xfAC
(and consequently Cz >> Cp), the error amplifier transfer function at 2xfAC can be
approximated to:
H 2( s ) ≅
g m ⋅ ( 1 + sRgm C Z )
sC Z
Since CZ has already been determined, only Rgm needs to be calculated:
H 2 ( j 2π ⋅ f AC ) = GVA − H 1 = −15dB = 0.177
2
Rgm
 G − H1  
1
 − 
=  VA
 g m   2π ⋅ 2 ⋅ f AC ⋅ CZ



2
Substituting fAC=47Hz, gm=49µS, CZ=0.56µF yields
R gm = 2kΩ
The location of the zero in the compensation scheme can now be estimated:
fz = 1/(2*π*Rgm.Cz) = 1/(2*π*2kohm*0.56µF) = 142Hz
The location of the pole in the power stage transfer function (assuming a resistive
load) is:
fPS = 1/(2*π*COUT*RL/2) = 1/[2*π*330uF*(385V*385V/350W)/2] = 2.3Hz
Since the location of zero is more than a decade away from that of the pole, it is
likely that this compensation scheme may result in low phase margin. This is
discussed more in “Phase Margin Discussion” in step 4.
Step 3: Choose Cp based on high-frequency pole location
The pole frequency should be chosen higher than the cross over frequency and
significantly lower than the switching frequency in order to attenuate switching
noise and switching frequency ripple in the output capacitor: typical value is 1/6
to 1/10 of the switching frequency. Choosing 1/6xfSW (=0.166*66kHz=11kHz) for
this converter:
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AN-1150
24
1
1
≅
Cz ⋅ Cp 2π ⋅ Rgm ⋅ Cp
2π ⋅ Rgm
Cz + Cp
1
= 7.32nF
Cp =
2π ⋅ 2kΩ ⋅ 66kHz ⋅ 0.166
f P0 =
Step 4: Estimate bandwidth & phase margin
The voltage loop response for 85VAC and 264VAC is plotted at full output power
condition of 350W in Fig.12. At 85VAC/350W the cross-over frequency is 5Hz
and phase margin is about 27°. At 264VAC/350W the cross-over frequency is
16Hz and phase margin is about 15°. This was anticipated considering the wide
separation between the zero and the pole locations. In this converter, due to the
low phase margin, the response to a load step can be oscillatory and may not be
acceptable in some applications. At lighter load conditions, the phase margin will
drop even further. However, there will be fast transient response. In the end the
trade-off between transient response and phase margin should be considered.
90
90
Gain 85VAC Uncompensated
Gain 85VAC Compensated
60
60
EA Gain
Phase 85VAC Uncompensated
EA Phase
0
Gain (dB)
30
Phase 85VAC Compensated
0
-30
-30
-60
-60
-90
-90
-120
-120
-150
-150
-180
0.01
90
0.1
1
10
100
f (Hz)
1000
10000
Phase (deg)
30
-180
100000
90
Gain 264VAC Uncompensated
Gain 264VAC Compensated
60
60
EA Gain
EA Phase
30
Phase 264VAC Uncompensated
30
Phase 264VAC Compensated
0
-30
-30
-60
-60
-90
-90
-120
-120
-150
-150
-180
0.01
0.1
1
10
100
1000
10000
Phase (deg)
Gain (dB)
0
-180
100000
f (Hz)
Fig.12: Overall Loop Gain at 85/264VAC & 350W (fast loop + low phase margin)
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AN-1150
25
Phase Margin Discussion:
The zero in the error amplifier compensation can provide phase boost to
compensate the phase lag due to the power stage pole. If the zero is more than a
decade away from the power stage pole there is minimal phase boost. The
location of the zero can be brought closer to the power stage pole by increasing
the value of Cz or Rgm or both. However, the trade-offs are as follows:
• Increasing Cz reduces the DC gain of the transfer function and slows
down the loop response (more sluggish response to a load step)
• Increasing Rgm increases the low frequency gain of the error amplifier
transfer function and hence the attenuation at 2xfAC may be insufficient to
meet the 0.5% requirement described earlier.
To illustrate the trade-offs, the following examples are presented with the goal of
improving the phase margin:
• Option 1: Increase the soft-start time. For example, if the soft-start time is
increased to 180ms (3x), then Cz=1.69uF, Rgm=3.49kohm, Cp=4.2nF. The
cross-over frequency and phase margin are 2.6Hz & 47° at 85VAC and 9.5Hz
and 33° at 264VAC as seen in Fig.13. Due to the higher Cz capacitor, the
transient response behavior is likely to be more sluggish for this
compensation arrangement.
90
90
Gain 85VAC Uncompensated
Gain 85VAC Compensated
60
60
EA Gain
Phase 85VAC Uncompensated
EA Phase
0
Gain (dB)
30
Phase 85VAC Compensated
0
-30
-30
-60
-60
-90
-90
-120
-120
-150
-150
-180
0.01
90
0.1
1
10
100
f (Hz)
1000
10000
Phase (deg)
30
-180
100000
90
Gain 264VAC Uncompensated
Gain 264VAC Compensated
60
60
EA Gain
EA Phase
30
Phase 264VAC Uncompensated
30
Phase 264VAC Compensated
0
-30
-30
-60
-60
-90
-90
-120
-120
-150
-150
-180
0.01
0.1
1
10
100
1000
10000
Phase (deg)
Gain (dB)
0
-180
100000
f (Hz)
Fig.13: Overall Loop Gain at 85/264VAC, 350W (slow loop + high phase margin)
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AN-1150
26
•
Option 2: At the expense of current distortion due to increased 2*fAC ripple in
VOUT, increase only the Rgm resistor while retaining the same soft-start time.
This has the effect of placing the zero closer to the pole in the power stage.
For example if H1(s).H2(s) attenuation at 2xfAC can be set at 1.5% instead of
0.5%. Then retaining Cz=0.56uF, we can recalculate Rgm=10kohm and
recalculate Cp=1.4nF. The cross-over frequency and phase margin are 5Hz &
35° at 85VAC and 20Hz and 42° at 264VAC as seen in Fig.14. While this may
cause some distortion (increased 3rd harmonic current), the EN61000-3-2
harmonic standards will still easily be met.
90
90
Gain 85VAC Uncompensated
Gain 85VAC Compensated
60
60
EA Gain
Phase 85VAC Uncompensated
EA Phase
0
Gain (dB)
30
Phase 85VAC Compensated
0
-30
-30
-60
-60
-90
-90
-120
-120
-150
-150
-180
0.01
0.1
1
10
100
1000
10000
Phase (deg)
30
-180
100000
f (Hz)
90
90
Gain 264VAC Uncompensated
Gain 264VAC Compensated
60
60
EA Gain
EA Phase
30
Phase 264VAC Uncompensated
30
Phase 264VAC Compensated
0
-30
-30
-60
-60
-90
-90
-120
-120
-150
-150
-180
0.01
0.1
1
10
100
1000
10000
Phase (deg)
Gain (dB)
0
-180
100000
f (Hz)
Fig.14: Overall Loop Gain at 85/264VAC, 350W (fast loop + high phase margin,
but possibly increased current distortion)
www.irf.com
AN-1150
27
•
Option 3: This is the compromise approach between option 1 & 2 and is left to
the user to pursue (for example using soft-start time=100ms & H1(s).H2(s)
attenuation at 2xfAC = 1%).
4. PFC Converter Physical Design & Layout Tips
4.1 Pin COM
Grounding is the most important layout consideration for PFC ICs. Some ICs
even have separate power ground and signal ground pins for better noise
immunity. Since IR1152 has only one ground pin, additional care is required
during board layout. The parasitic inductance and capacitance in the power
ground trace usually generates a lot of noise because of high RMS currents and
‘dV/dt’s & ‘dI/dt’s from switching loops. There is also the possibility of high
common-mode currents that is to be considered for certain types of loads (such
as motor drive inverters). This is illustrated in Fig.15. The control circuitry of the
IC has to be shielded from this noise as much as possible.
-
+
1
2
3
4
COM GATE
COMP VCC
ISNS
VFB
BOPOVP/EN
8
7
6
5
These traces carry high frequency current
Easy to generate noise with parasitic inductance
Fig.15: – Noise in power ground (BAD connection practice)
A few rules are listed below which can improve the system noise immunity.
• COM Rule 1: A STAR-connection is highly recommended in PFC converter
layout for the power GND, IC COM & MOSFET source nodes. In the starconnection, the IC COM pin, the current sense resistor and source of PFC
switch are connected at one single point as illustrated in Fig.16. If a ground
plane is used, it is important to ensure that the ground plane does not conduct
currents. So the ground plane is also connected to the STAR-connection
point only.
In terms of the control circuitry, the best approach is to provide each control loop
of the IC with a dedicated return path and have an independent star-connection
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AN-1150
28
to IC COM pin. However, in reality, sometimes it is difficult to do so due to the
limitation of PCB space and hence it is useful to apply some rules:
• COM Rule 2: Separate the VCC and Gate-drive loop return paths to COM
from all other control circuit loops (The gate drive loop and VCC loop are the
noisiest of all control circuit loops. Both carry high-frequency switching
currents for turning the PFC switch on/off).
• COM Rule 3: VCOMP voltage is the control voltage for the feedback loop from
which the oscillator of the IC is also derived. Hence the return path of the
COMP loop is very important in IR1152. It is recommended to provide the
COMP control loop with a dedicated return path to COM pin (as shown in
Fig.18 in “Pin COMP” rules section next).
• COM Rule 4: VFB, OVP & BOP control loops can share the same return path
to COM.
• COM Rule 5: The star connection point must be as close to the IC as
physically possible.
These rules are illustrated in Fig.17.
AC Line
Bridge
-
+
LBST
DBST
AC Neutral
CIN
RBOP1
CVCC
CZ
RBOP2
CP
1
Rgm
2
3
4
RBOP3
COM GATE
COMP VCC
ISNS
VFB
BOPOVP/EN
8
RVFB1
ROVP1
RVFB2
ROVP2
RG
7
COUT
MBST
6
5
CBOP
RVFB3
ROVP3
CSF
IC COM, PFC switch SOURCE
& RSNS Star Connection
RSF
RSNS
GND
Fig.16: STAR-Connection for system ground, GND
www.irf.com
AN-1150
29
AC Line
Bridge
-
+
LBST
AC Neutral
COMP Loop
Return trace
CIN
DBST
VCC Loop
Return trace
RBOP1
CVCC
CZ
RBOP2
CP
1
Rgm
2
STAR
CONNECTION
3
4
RBOP3
CBOP
COM GATE
COMP VCC
ISNS
VFB
BOPOVP/EN
RVFB1
ROVP1
RVFB2
ROVP2
RG
8
6
5
RVFB3
VFB, OVP & BOP
Loop Return trace
CSF
COUT
MBST
7
ROVP3
Gate Loop
Return trace
RSF
RSNS
GND
Fig.17: 3 IC control loops with STAR connection to COM
4.2 Pin COMP
The COMP pin is the most important control pin in IR1152. VCOMP voltage is the
control voltage for the feedback loop from which the oscillator of the IC is also
derived. It is very important to follow the 2 rules below to maintain a stable
feedback loop and stable oscillator.
COMP RULE 1: Place the CZ, CP & Rgm components close to COMP pin.
COMP RULE 2: Keep the compensation loop of IR1152 fully independent from
all other control circuit loops (don’t share ground return race of COMP loop with
other control loops)
It is for these reasons that the COMP is located right next to the COM pin to
facilitate easy, isolated routing of the COMP control loop. These rules are
illustrated in Fig.18 below.
CVCC
CZ
CP
1
Rgm
2
3
4
COM GATE
COMP VCC
ISNS
VFB
BOPOVP/EN
CBOP
Fig. 18: Fully isolated COMP control loop
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4.3 Pin ISNS
Current sensing is always tough in PFC converters, because the signal level is
low while environment is noisy. Further, common mode currents tend to
preferentially flow through the current sense line rather than the boost inductor
line, because of the high-frequency impedance offered by the boost inductor. The
ISNS pin also needs one-point connection to the negative side of current sense
resistor through a current-limiting series resistor. If RC filtering is to be performed
for VISNS, place the filter capacitor CSF close to the current sense resistor (rather
than close to the IC) as shown Fig.19 in order to filter the noise at the source.
RBOP1
CVCC
CZ
RBOP2
CP
1
Rgm
2
3
4
RBOP3
COM GATE
COMP VCC
ISNS
VFB
BOPOVP/EN
8
7
6
5
CBOP
CSF
RC filtering close to the
current sense resistor
RSF
RSNS
GND
Fig.19: ISNS connection with RC filter close to the RSNS resistor
Use non-inductive resistor (metal strip or film type) for current sensing to avoid
high di/dt transient noise. Do not use wirewound type resistor.
4.4 Pins BOP, OVP/EN & VFB
BOP pin will have a capacitor (100nF or so) tied between the pin & COM. So this
pin is relatively noise immune. The OVP and VFB loops are very similar with
option of using a stabilization capacitor of few hundred pF, if needed. These two
pins will sense output voltage through resistor divider whose high side resistance
is about 1-2Mohm & low side resistance is around few tens of kohm. This high
impedance between these pins and COM makes them less immune to noise. So
it is very important to route the VFB & OVP/EN traces & place the resistor divider
components away from high dV/dt or high dI/dt power traces like Drain of
MOSFET, Gate driver loop, current sense trace & boost inductor. As mentioned
earlier, it is ok for VFB, OVP & BOP control loop return paths (to COM) to share
the same trace, since the signals are near-DC on all these pins.
Recall that OVP pin also performs enable function which must be protected from
spurious trigger. Adding a small capacitor to OVP pin is recommended. The
capacitance cannot be too high since it will affect OVP response time. Normally a
50-100pF cap is good enough to reduce noise while not affecting OVP transient
response.
4.5 Pin VCC
A 1uF VCC decoupling capacitor (ceramic SMT capacitor with low ESR) should be
placed between VCC & COM pins as close as possible to the IC to minimize the
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loop inductance. The ideal location is right on top of the IC as shown in Fig.20.
As long as this decoupling capacitor is placed close to the IC, the other bulk VCC
capacitor (tens of uF, not shown in Fig.20) which is usually provided can be
connected anywhere near the IC. Remember to separate the VCC loop return
path (to COM) from the other control loops as it carries the high-frequency
current supplying gate charge to drive the PFC switch.
SMD capacitor placed
very close to IC
CVCC
CZ
CP
1
Rgm
2
3
4
COM GATE
COMP VCC
ISNS
VFB
BOPOVP/EN
8
RG
7
6
5
Fig. 20: Vcc decoupling capacitor placed right on top of the IC with tight routing
4.6 Pin Gate
IR1152 GATE output can drive the PFC switch directly or be used with a gate
drive buffer. Minimize the length of gate drive loop to reduce the parasitic
inductance, that can limit the peak current otherwise place the gate drive buffer
close to the switching MOSFETs to achieve fast switching. Also, it’s a good
practice to choose a bigger gate turn-on resistor and slow down the turning-on
speed of MOSFET in order to limit dI/dt & reverse recovery current peaks. Of
course, the trade-off with turn-on switching losses must be considered.
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