AN-9736 [FAIRCHILD]

Design Guideline of AC-DC Converter Using FL6961, FL6300A for 70W LED Lighting; 的AC -DC转换器的设计准则采用FL6961 , FL6300A为70W的LED照明
AN-9736
型号: AN-9736
厂家: FAIRCHILD SEMICONDUCTOR    FAIRCHILD SEMICONDUCTOR
描述:

Design Guideline of AC-DC Converter Using FL6961, FL6300A for 70W LED Lighting
的AC -DC转换器的设计准则采用FL6961 , FL6300A为70W的LED照明

转换器
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中文:  中文翻译
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www.fairchildsemi.com  
AN-9736  
Design Guideline of AC-DC Converter Using FL6961 &  
FL6300A for 70W LED Lighting  
switching (ZVS) or near-ZVS (also called valley switching)  
of boost switch. The QR flyback converter for the DC-DC  
conversion achieves higher efficiency than the conventional  
hard-switching converter with valley switching.  
Summary  
This application note describes a design strategy for a Power  
Factor Correction (PFC) circuit and higher-power  
conversion efficiency using FL6961 and FL6300A. Based  
on this design guideline and several functions of each  
controller for LED lighting applications, a design example  
with detailed parameters demonstrates the performance.  
The FL6961 provides a controlled on-time to regulate the  
output DC voltage and achieves natural power factor  
correction. The maximum on-time of the switch is  
programmable to ensure safe operation during AC  
brownouts. The FL6300A ensures  
thepower system  
Introduction  
operates in quasi-resonant operation in wide range line  
voltage and reduces switching loss to minimize switching  
voltage in drain of the power MOSFET. To minimize  
standby power consumption and improve light-load  
efficiency, a proprietary Green-Mode provides off-time  
modulation to decrease switching frequency and perform  
extended valley voltage switching to keep to a minimum  
switching voltage.  
Figure 1 shows the typical application circuit, with the BCM  
PFC converter in the front end and the Quasi-resonant (QR)  
flyback converter in the back end. FL6961 and FL6300A  
achieve high efficiency with relatively low cost for  
75~200W applications where BCM and QR operation with  
a single switch shows best performance. BCM boost PFC  
converter can achieve better efficiency with lower cost than  
Continuous Conduction Mode (CCM) boost PFC converter.  
These benefits result from the elimination of the reverse-  
recovery losses of the boost diode and zero-voltage  
Figure 1. Typical Application Circuit  
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
AN-9736  
APPLICATION NOTE  
and output capacitor CO. The inductor current IL can be  
expressed as:  
1. Basin Operation of BCM Boost  
PFC Converter  
The typical boost converter and its operational waveforms  
are shown in Figure 2, Figure 3, and Figure 4.  
VꢉVꢀtꢃ  
(2)  
ILꢀtꢁꢈꢈꢃ ꢄ  
ꢇ  
The on-time of the power MOSFET Q is determined by the  
output of the error amplifier that monitors the pre-regulator  
output voltage. With a low-bandwidth error amplifier, the  
feedback signal is almost constant during a half AC cycle,  
resulting a fixed on-time of the power MOSFET at a  
specific AC voltage and some certain output power level.  
Therefore, the peak inductor current ILpk automatically  
follows the input voltage Vg(t), achieving a natural power  
factor correction mechanism. Figure 5 shows the typical  
inductor current waveform during a half AC cycle.  
vL (t)   
D
Lb  
iL (t)  
Vo  
vg (t)  
Q
Co  
Ro  
Figure 2. Boost Converter  
vL (t)   
iL (t)  
vL (t)   
iL (t)  
Lb  
Lb  
vo  
vg (t)  
vg (t)  
Q
Ro  
Co  
(a) Switch Q is ON  
(b) Switch Q is OFF  
Figure 3. Switching Sequences of the Boost Converter  
vL (t)  
vg (t)  
vo vg (t)  
vg (t) vo vg (t)  
iL (t)  
Lb  
Lb  
Figure 5. Controlled On-Time Inductor Current Waveform  
iL,avg (t)  
Referring to Figure 4, considering one switching period the  
average inductor current, IL,ave(t) can be calculated by the  
average area of triangle waveform of inductor current:  
Q
tꢁꢂ  
ton  
toff  
ꢎ  
ꢀ ꢃꢎ  
Vt  
Tꢑ  
(3)  
ꢀ ꢃ  
ꢀ ꢃ  
IL,ꢊꢋꢅ t ꢄ ꢌVt ꢍ  
ꢏ ꢐ  
ꢀ ꢃ  
· Tꢑ  
VꢉVt  
2 · ꢆꢇ  
Figure 4. One-Cycle Waveform of the Boost Converter  
1.1. Operation Principle  
When Q turns on, the rectifier diode D is reverse-biased and  
output capacitor CO supplies load current. The rectified AC  
line input voltage Vg(t) is applied to the inductor Lb so that  
inductor current IL ramps up linearly and can be expressed  
as:  
Vꢀtꢃ  
(1)  
ILꢀtꢁꢂꢃ ꢄ  
ꢇ  
When Q turns off, the voltage VO-Vg(t) is applied to  
inductor Lb and the polarity on the inductor Lb is reversed.  
The diode D is forward-biased in this stage. The energy  
stored in the inductor Lb is delivered to supply load current  
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
2
AN-9736  
APPLICATION NOTE  
2. Operation Principle of Quasi-  
Resonant Flyback Converter  
QR flyback converter topology can be derived from a  
conventional square wave, Pulse-Width Modulated (PWM),  
flyback converter without additional components. Figure 6  
and Figure 7 show the simplified circuit diagram of a quasi-  
resonant flyback converter and its typical waveforms.  
Figure 7. Typical Waveforms of QR Flyback Converter  
Figure 6. Schematic of QR Flyback Converter  
2.1. Operation Principle  
3. Design Considerations  
.
During the MOSFET on time (tON), input voltage  
(VIN) is applied across the primary-side inductor  
(Lm). MOSFET current (IDS) increases linearly  
from zero to the peak value (Ipk). During this time,  
the energy is drawn from the input and stored in  
the inductor.  
This design procedure uses the schematic in Figure 1 as a  
reference. A 70W PFC application with universal input  
range is selected as a design example. The design  
specifications are:  
.
.
.
.
.
.
Line Voltage Range: 90~277VAC (60Hz)  
Output of DC-DC Converter: 24V/2.9A (70W)  
PFC Output Voltage for Line Voltage: 420V  
Minimum PFC Switching Frequency: > 58kHz  
Minimum QR flyback Switching Frequency: > 50kHz  
Overall Efficiency: 90% (PFC: 95%, QR: 95%)  
.
When the MOSFET is turned off, the energy stored  
in the inductor forces the rectifier diode (D) to turn  
on. During the diode ON time (tD), the output  
voltage (Vo) is applied across the secondary-side  
inductor and the diode current (ID) decreases  
linearly from the peak value to zero. At the end of  
tD, all the energy stored in the inductor has been  
delivered to the output. During this period, the  
output voltage is reflected to the primary side as  
VONP/NS. Then, the sum of input voltage (VIN)  
and the reflected output voltage (VoNP/NS) is  
imposed across the MOSFET.  
3.1. PFC Section  
3.1.1. Boost Inductor Design  
The boost inductor value is determined by the output power  
and the minimum switching frequency. The voltage-second  
balance equation for the inductor is:  
.
When the diode current reaches zero, the drain-to-  
source voltage (VDS) begins to oscillate by the  
resonance between the primary-side inductor (Lm)  
and the MOSFET output capacitor (COSS) with an  
amplitude of VONP/NS on the offset of VIN, as  
depicted in Figure 7. Quasi-resonant switching is  
achieved by turning on the MOSFET when VDS  
reaches its minimum value. This reduces the  
MOSFET turn-on switching loss caused by the  
capacitance loading between the drain and source  
of the MOSFET.  
(4)  
(5)  
V ꢀtꢃ · tON ꢄ ꢀVO.PFC ꢉ V ꢀtꢃꢃ · tOFF  
ꢒN  
ꢒN  
1
1
VO.PFC ꢉ 2V  
LꢒNE  
fSW,  
·
MꢒN  
t
ON ꢍ tOFF tON  
VO.PFC  
where VIN(t) is the rectified line voltage.  
LINE is RMS line voltage;  
ON is the MOSFET conduction time; and  
VO.PFC is the PFC output voltage.  
V
t
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
3
AN-9736  
APPLICATION NOTE  
The MOSFET conduction time with a given line voltage at a  
nominal output power is given as:  
(Design Example) Since the output voltage is 420V for line  
voltage, the minimum frequency occurs at high-line  
(277VAC) and full-load condition. Assuming the overall  
efficiency is 90% and selecting the minimum frequency as  
58kHz, the inductor value is obtained as:  
2 · OUꢔ · ꢆ  
tON  
(6)  
η · VLꢒNE  
where:  
is the overall efficiency;  
L is the boost inductance; and  
POUT is the nominal output power.  
η · VLꢒNE MAX  
VO.PFC ꢉ 2V  
LꢒNE MAX  
ꢆ ꢄ  
·
2 · OUꢔ · fSW. MꢒN  
VO.PFC  
0.9 · 277 ꢎ  
420 ꢉ 2 · 277  
Using Equation 5, the minimum switching frequency of  
Equation 6 can be expressed as:  
·
ꢄ 570µH  
2 · 70 · 58 ꢐ 10ꢛ  
420  
The maximum peak inductor current at nominal output  
power is calculated as:  
η · VLꢒNE  
VO.PFC ꢉ 2V  
LꢒNE  
fSW.  
·
(7)  
MꢒN  
2 · OUꢔ · ꢆ  
VO.PFC  
2 2 · ꢓ  
2 2 · 70  
OUꢔ  
IL.PK  
ꢄ 2.44 ꢘ  
As shown in Figure 5, considering one AC line voltage  
cycle, the minimum switching frequency occurs at peak of  
the AC line voltage. Also, the minimum switching  
frequency may occur in AC maximum or minimum input  
voltage, depending on the output voltage. Therefore,  
calculate both the maximum and the minimum input voltage  
and choose the lower inductance value. Once the output  
voltage and minimum switching frequency are set, the  
inductor value is given as:  
η · VLꢒNE.MꢒN 0.9 ꢐ 90  
2 · OUꢔ · ꢆ  
2 · 70 · 570 ꢐ 10ꢜꢝ  
0.9 ꢐ 90 ꢎ  
MAX  
tON  
η · VLꢒNE MꢒN  
ꢄ 10.9µs ꢕ 20µs  
Assuming RM10 core (PC40, Ae=85mm2) is used and  
setting B as 0.25T, the primary winding should be:  
I
L.PK · ꢆ 2.44 · 570 ꢐ 10ꢜꢝ  
ꢄ ꢄ 65.8 turns  
BOOSꢔ  
85 ꢐ 10ꢜꢝ ꢐ 0.25  
· Δꢚ  
η · VLꢒNE MAX  
VO.PFC ꢉ 2V  
LꢒNE MAX  
(8)  
ꢆ ꢄ  
·
2 · OUꢔ · fSW. MꢒN  
VO.PFC  
Thus, the number of turns (NBOOST) of boost inductor is  
determined as 65.  
where VLINE,MAX is the maximum line voltage.  
As the minimum frequency decreases, the switching loss is  
reduced, while the inductor size and line filter size increase.  
Thus, the minimum switching frequency should be  
determined by the trade-off between efficiency and the size  
of magnetic components. The minimum switching  
frequency must be above 20kHz to prevent audible noise.  
3.1.2. Auxiliary Winding Design  
Figure 9 shows the internal block for Zero-Current  
Detection (ZCD) for the PFC. FL6961 indirectly detects the  
inductor zero-current instant using an auxiliary winding of  
the boost inductor. The auxiliary winding should be  
designed such that the voltage of the ZCD pin rises above  
2.1V when the boost switch is turned off to trigger internal  
comparator as:  
Once the inductance value is decided, the maximum peak  
inductor current at the nominal output power is obtained at  
low-line condition as:  
ZCD  
ꢀVO.PFC ꢉ 2VLꢒNE.MAXꢃ ꢞ 2.1V  
(12)  
BOOSꢔ  
2 2 · ꢓ  
OUꢔ  
IL.PK  
(9)  
η · VLꢒNE.MꢒN  
The ZCD pin has upper voltage clamping and lower voltage  
clamping at 10V and 0.3V, respectively. When the ZCD pin  
voltage is clamped at 0.3V, the maximum sourcing current  
is 1.5mA and, therefore, the resistor RZCD should be  
properly designed to limit the current of the ZCD pin below  
1.5mA in the worst case as:  
where VLINE,MIN is the minimum line voltage.  
Since the maximum on time is internally limited at 25µs, it  
should be smaller than 25µs, as calculated by:  
2 · OUꢔ · ꢆ  
MAX  
tON  
ꢕ 20µs  
(10)  
V
AUX  
2V  
AUX  
ꢒN  
LꢒNE.MAX  
η · VLꢒNE MꢒN  
(13)  
RZCD  
·
·
1.5mꢘ ꢖBOOSꢔ  
1.5mꢘ  
BOOSꢔ  
The number of turns of the boost inductor should be  
determined considering the core saturation. The minimum  
number is given as:  
I
L.PK · ꢆ  
BOOSꢔ  
(11)  
· Δꢚ  
where is Ae is the cross-sectional area of core and B is  
the maximum flux swing of the core in Tesla. B should  
be set below the saturation flux density.  
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
4
AN-9736  
APPLICATION NOTE  
3.1.3. Current-Sensing Resistor for PFC  
FL6961 has pulse-by-pulse current limit function. It is  
typical to set the pulse-by-current limit level at 20~30%  
higher than the maximum inductor current:  
0.82  
RCSꢟ  
(14)  
I
L.PKꢀ1 ꢍ ꢠMAꢡGꢒNꢃ  
where KMARGIN is the margin factor and 0.85V is the  
pulse-by-pulse current limit threshold.  
(Design Example) Choosing the margin factor as 35%, the  
sensing resistor is selected as:  
0.85  
0.82  
RCSꢟ  
ꢄ 0.25Ω  
IL.PKꢀ1 ꢍ ꢠMAꢡGꢒN  
2.44ꢀ1 ꢍ 0.35ꢃ  
Figure 8. Internal Block for ZCD  
3.1.4. Output Capacitor Selection  
For a given minimum PFC output voltage during the hold-  
up time, the PFC output capacitor is obtained as:  
2OUꢔ · tꢣOLD  
VO.PFC ꢉ VO.PFC.ꢣLD  
O.PFC  
(15)  
where:  
OUT is total nominal output power;  
tHOLD is the required holdup time; and  
VO.PFC,HLD is the allowable minimum output voltage  
during the hold-up time.  
P
NZCD  
(VO.PFC VIN  
)
NBOOST  
NZCD  
VIN  
For PFC output capacitor, it is typical to use 0.5~1µF per  
1W output power for 420V PFC output. Meanwhile, it is  
reasonable to use about 1µF per 1W output power for  
variable output PFC due to the larger voltage drop during  
the hold-up time than 420V output.  
NBOOST  
(Design Example) Assuming the minimum allowable PFC  
output voltage during the hold-up time is 160V, the  
capacitor should be:  
Figure 9. ZCD Waveforms  
2OUꢔ · tꢣOLD  
VO.PFC ꢉ VO.PFC.ꢣLD  
2 · 80 · 20 ꢐ 10ꢜꢛ  
420 ꢉ 350 ꢎ  
(Design Example) The number of turns for the auxiliary  
ZCD winding is obtained as:  
O.PFC  
ꢄ 60µꢤ  
2.1ꢖBOOSꢔ  
ZCD  
ꢄ 4.83 turn  
ꢀVO.PFC ꢉ 2VLꢒNE.MAXꢃ  
A 68F capacitor is selected for the output capacitor.  
With a margin, NAUX is determined as 6 turns.  
ZCD is selected from:  
2V  
3.1.5. Design Compensation Network  
The feedback loop bandwidth must be lower than 20Hz for  
the PFC application. If the bandwidth is higher than 20Hz,  
the control loop may try to reduce the 120Hz ripple of the  
output voltage and the line current is distorted, decreasing  
power factor. A capacitor is connected between COMP and  
GND to attenuate the line frequency ripple voltage by 40dB.  
If a capacitor is connected between the output of the error  
amplifier and the GND, the error amplifier works as an  
integrator and the error amplifier compensation capacitor  
can be calculated by:  
R
AUX  
2 · 277  
6
LꢒNE.MAX  
RZCD  
·
·
ꢄ 24kΩ  
1.5mꢘ  
BOOSꢔ 1.5 ꢐ 10ꢜꢛ 65  
as 30k.  
100 · gM  
25  
COMP  
·
(16)  
2π · 2fLꢒNE VO.PFC  
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
5
AN-9736  
APPLICATION NOTE  
To improve the power factor, CCOMP must be higher than the  
calculated value. However, if the value is too high, the  
output voltage control loop may become slow.  
(Design Example)  
100 · gM  
2.5  
COMP  
·
2π · 2fLꢒNE VO.PFC  
100 · 125 ꢐ 10ꢜꢝ 2.5  
·
ꢄ 100nꢤ.  
2π · 2 · 60  
420  
470nF is selected for better power factor.  
3.2. DC-DC Section  
3.2.1. Determine the Reflected Output Voltage (VRO  
)
Figure 10 shows the typical operation waveforms of a quasi-  
resonant flyback converter. When the MOSFET is turned  
off, the input voltage (PFC output voltage), together with  
the output voltage reflected to the primary (VRO), is imposed  
on the MOSFET. When the MOSFET is turned on, the sum  
of input voltage reflected to the secondary side and the  
output voltage is applied across the diode. Thus, the  
maximum nominal voltage across the MOSFET (VDS.nom  
)
and diode are given as:  
ꢂꢁꢥ  
ꢀ ꢃ  
ꢄ VO.PFC ꢍ n VO ꢍ VF ꢄ VO.PFC ꢍ VꢡO  
(17)  
VDS  
where:  
VꢡO  
Figure 10.Typical Waveforms of QR Flyback Converter  
(18)  
n ꢄ  
VO ꢍ VF  
(Design Example) Assuming 650V MOSFET and 150V  
Diode are used for primary side and secondary side,  
respectively, with 18% voltage margin:  
VO.PFC  
n
V
O.PFC ꢀ  
ꢂꢁꢥ  
VD  
ꢄ VO ꢍ  
ꢄ VO ꢍ VO ꢍ VF  
(19)  
VꢡO  
ꢂꢁꢥ  
By increasing VRO (i.e. the turns ratio, n), the capacitive  
switching loss and conduction loss of the MOSFET are  
reduced. This also reduces the voltage stress of the  
secondary-side rectifier diode. However, this increases the  
voltage stress on the MOSFET. Therefore, VRO should be  
determined by a trade-off between the voltage stresses of the  
MOSFET and diode. It is typical to set VRO such that  
0.82 · 650V ꢞ VDS  
ꢄ VO.PFC ꢍ VꢡO  
ꢦ VꢡO ꢕ 0.82 · 650 ꢉ VO.PFC ꢄ 133V  
V
O.PFC ꢀ  
VO ꢍ VF  
ꢂꢁꢥ  
0.82 · 150 ꢞ VDS  
ꢄ VO ꢍ  
VꢡO  
VO.PFC  
ꢂꢁꢥ  
ꢀ ꢃ  
VO ꢍ VF ꢄ 106V  
ꢦ VꢡO ꢞ VDS  
0.82 · 150 ꢉ VO  
V
DS.nom and VD.nom are 75~85% of their voltage ratings.  
V
RO is determined as 130V.  
3.2.2. Transformer Design  
Figure 11 shows the typical switching timing of a quasi-  
resonant converter. The sum of MOSFET conduction time  
(tON), diode conduction time (tD), and drain voltage falling  
time (tF) is the switching period (tS). To determine the  
primary-side inductance (Lm), the following parameters  
should be determined first.  
Minimum Switching Frequency (fS.QRmin  
)
The minimum switching frequency occurs at the minimum  
input voltage and full-load condition, which should be  
higher than 20kHz to avoid audible noise. By increasing  
fS.QRmin, the transformer size can be reduced. However, this  
results in increased switching losses. Determine fS.QRmin by a  
trade-off between switching losses and transformer size.  
Typically fS.QRmin is set to around 50kHz.  
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
6
AN-9736  
APPLICATION NOTE  
Falling Time of the MOSFET Drain Voltage (tF)  
As shown in Figure 11, the MOSFET drain voltage fall time  
is half of the resonant period of the MOSFET’s effective  
output capacitance and primary-side inductance. The typical  
value for tF is 0.6~1.2µs.  
Non-Conduction Time of the MOSFET (tOFF  
)
FL6300A has a minimum non-conduction time of MOSFET  
(8µs), during which turning on the MOSFET is prohibited.  
To maximize the efficiency, it is necessary to turn on the  
MOSFET at the first valley of MOSFET drain-to-source  
voltage at heavy-load condition. Therefore, the MOSFET  
non-conduction time at heavy load condition should be  
larger than 8µs.  
Although QR flyback is operated in PFC end for normal  
operation; when Dmax is calculated to meet all input  
conditions, it should take into account the minimum input  
voltage of VLINE due to the start sequence between PFC and  
QR flyback at startup.  
After determining fS.QRmin and tF, the maximum duty cycle is  
calculated as:  
Figure 11.Switching Timing of QR Flyback Converter  
When designing the transformer, the maximum flux density  
(B) swing in normal operation as well as the maximum flux  
density (Bmax) in transient should be considered. The  
maximum flux density swing in normal operation is related  
to the hysteresis loss in the core, while the maximum flux  
density in transient is related to the core saturation.  
VꢡO  
ꢥꢪꢂ  
ꢥꢊꢨ  
ꢩ1 ꢉ fS.Qꢡ  
· tFꢫ  
(20)  
VLꢒNE ꢍ VꢡO  
The minimum number of turns for the transformer primary  
side to avoid over temperature in the core is given by:  
The primary-side inductance is obtained as:  
PK  
· IDS  
ꢥꢪꢂ  
(25)  
P  
ηQꢡ · ꢀVLꢒNE · ꢧꢥꢊꢨꢎ  
· Δꢚ  
(21)  
ꢥ  
ꢥꢪꢂ  
2 · fS.Qꢡ  
· OUꢔ  
where B is the maximum flux density swing in Tesla. If  
there is no reference data, use B =0.25~0.30T.  
Once Lm is determined, the maximum peak current and  
RMS current of the MOSFET in normal operation are  
obtained as:  
Once the minimum number of turns for the primary side is  
determined, calculate the proper integer for NS so that the  
min  
resulting NP is larger than NP  
as:  
V
LꢒNE · ꢧꢥꢊꢨ  
PK  
IDS  
(22)  
(23)  
ꢥꢪꢂ  
· fS.Qꢡ  
ꢥꢪꢂ  
(26)  
P ꢄ n · ꢖS ꢞ ꢖP  
ꢥꢊꢨ  
3
ꢡMS  
PKꢬ  
ꢄ IDS  
The number of turns of the auxiliary winding for VDD is  
given as:  
IDS  
VDDꢂꢁꢥ ꢍ V  
The MOSFET non-conduction time at heavy load is  
obtained as:  
AUX  
FA · ꢖS  
(27)  
VO ꢍ VF  
nom  
ꢀ1 ꢉ ꢧꢥꢊꢨꢃ  
where VDD is the nominal VDD voltage, typically 18V,  
and VFA is forward-voltage drop of VDD diode.  
tOFF  
(24)  
ꢥꢪꢂ  
fS.Qꢡ  
Once the number of turns of the primary winding is  
determined, the maximum flux density when the drain  
current reaches its pulse-by-pulse current limit level should  
be checked to guarantee the transformer is not saturated  
during transient or fault condition.  
To guarantee the first valley switching at heavy-load  
condition, tOFF should be larger than 8µs.  
The maximum flux density (Bmax) when drain current  
reaches IDS PK is given as:  
PK  
· IDS  
(28)  
ꢥꢊꢨ  
ꢕ ꢚꢑꢊꢭ  
· ꢖP  
Bmax should be smaller than the saturation flux density. If  
there is no reference data, use Bsat =0.35~0.40T.  
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
7
AN-9736  
APPLICATION NOTE  
(Design Example) Setting the minimum frequency is  
50kHz and the falling time is 0.8µs:  
VꢡO  
ꢥꢪꢂ  
ꢥꢊꢨ  
ꢩ1 ꢉ fS.Qꢡ  
· tFꢫ  
ꢜꢝꢃ  
VLꢒNE ꢍ VꢡO  
130  
127 ꢍ 130  
ꢥ  
1 ꢉ 50 ꢐ 10 · 0.8 ꢐ 10  
ꢄ 0.48  
ηQꢡ · ꢀVLꢒNE · ꢧꢥꢊꢨꢎ  
Figure 12. Detection Pin Section  
ꢥꢪꢂ  
2 · fS.Qꢡ  
· OUꢔ  
First, determine the ratio of the voltage divider resisters. The  
ratio of the divider determines what output voltage level to  
stop gate. In Figure 13, the sampling voltage VS is:  
0.95 · ꢀ127 · 0.48ꢃꢎ  
2 · 50 ꢐ 10· 70  
ꢄ 500μꢤ  
127 · 0.48  
500 ꢐ 10ꢜꢝ · 50 ꢐ 10ꢛ  
PK  
RA  
VS A · VO ·  
ꢕ 2.5V  
(29)  
IDS  
ꢄ 2.52ꢘ  
S  
RDEꢔ ꢍ RA  
ꢀ1 ꢉ ꢧꢥꢊꢨ  
1 ꢉ 0.48  
50 ꢐ 10ꢛ  
where NA is the number of turns for the auxiliary winding  
and NS is the number of turns for the secondary winding.  
tOFF  
ꢄ 10µs  
ꢥꢪꢂ  
fS.Qꢡ  
Assuming EER3124 (Ae=102mm2) core is used and the  
flux swing is 0.29T  
Figure 14 shows the internal valley detection block and the  
output voltage OVP detection block of FL6300A using  
auxiliary winding to detect VO. The internal timer  
(minimum tOFF time) prevents the system frequency from  
being too high. First valley switching is activated after  
minimum tOFF time of 8μs.  
PK  
· IDS  
· Δꢚ  
500 ꢐ 10ꢜꢝ · 2.52  
102 ꢐ 10ꢜꢝ · 0.29  
ꢥꢪꢂ  
P  
ꢄ 41.8  
ꢥꢪꢂ  
P ꢄ n · ꢖS ꢄ 5.3 · 8 ꢄ 42.4 ꢞ ꢖP  
The nominal voltage of VS is designed around 80% of the  
reference voltage 2.5V; thus, the recommended value for VS  
is 1.9V~2.1V. The output over-voltage protection works by  
the sampling voltage after the switching-off sequence. A  
4μs blanking time ignores the leakage inductance ringing. If  
the DET pin OVP is triggered, the power system enters latch  
mode until AC power is removed.  
VDDꢂꢁꢥ ꢍ V  
18 ꢍ 1.2  
24.5  
AUX  
FA · ꢖS ꢄ  
· 8 ꢄ 6.3  
VO ꢍ VF  
Assuming the pulse-by-pulse current limit for PFC output  
voltage is 120% of peak drain current at heavy load:  
PK  
· IDS  
· ꢖP  
500 · 2.52 · 1.2  
102 · 42  
ꢥꢊꢨ  
ꢄ 0.34T  
3.2.3. Design the Valley Detection Circuit  
Figure 12 shows the DET pin circuitry. The DET pin is  
connected to an auxiliary winding by RDET and RA. The  
voltage divider is used for the following purposes:  
.
Detect the valley voltage of the switching waveform for  
valley voltage switching. This ensures QR operation,  
minimizes switching losses, and reduces EMI.  
.
Produce an offset to compensate the threshold voltage  
of the peak current limit to provide a constant power  
limit. The offset is generated in accordance with the  
input voltage with the PWM signal enabled.  
Figure 13.Voltage Sampled After 4µs Blanking Time  
After Switch-Off Sequence  
.
A voltage comparator and a 2.5V reference voltage  
provide output OVP. The ratio of the divider  
determines the output voltage level to stop the gate.  
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
8
AN-9736  
APPLICATION NOTE  
(Design Example) Choosing the margin factor as 35%, the  
sensing resistor is selected as:  
0.8  
0.8  
RCSꢟ  
ꢄ 0.23Ω  
IDSPKꢀ1 ꢍ ꢠMAꢡGꢒN  
2.52ꢀ1 ꢍ 0.35ꢃ  
3.2.5. Design the Feedback Circuit  
Figure 15 is a typical feedback circuit mainly consisting of a  
op-amp and a photo-coupler. RH and RL form a voltage  
divider for output voltage regulation. RF and CF are adjusted  
for control-loop compensation. A small-value RC filter (e.g.  
RFB = 100, CFB = 1nF) placed from the FB pin to GND can  
increase stability substantially. The maximum source  
current of the FB pin is about 1.2mA. The phototransistor  
must be capable of sinking this current to pull the FB level  
down at no load. The value of the biasing resistor, RBIAS, is  
determined as:  
V
OP ꢉ VOPD  
· ꢢTR ꢞ 1.2 ꢐ 10ꢜꢛ  
(31)  
RBꢒAS  
where VOPD is the drop voltage of photodiode, about  
1.2V; VOP is the output voltage of operational amplifier  
(assuming about 2.5V); and CTR is the current transfer  
rate of the opto-coupler.  
Figure 14. Output Voltage Detection Block  
Once the secondary-side switching current discharges to  
zero, a valley signal is generated on the DET pin. It detects  
the valley voltage of the switching waveform to achieve the  
valley voltage switching. When the voltage of auxiliary  
winding VAUX is negative (as defined in Figure 12), the DET  
pin voltage is clamped to 0.3V. RDET is recommended as  
150kto 220kto achieve valley voltage switching. After  
the platform voltage VS in Figure 13 is determined, RA can  
be calculated by Equation 14.  
(Design Example) Setting RDET is 200kΩ and VS is around  
80% of the reference voltage 2.5V:  
Figure 15. Feedback Circuit  
The constant voltage and current output is adapted by  
measuring the actual output voltage and current with some  
external passive components and op-amp in the reference  
board. Because the output load, the High Bright LED (HB  
LED), and some passive components effect the ambient  
temperature, use the feedback path for stable operation.  
RA  
VS A · VO ·  
ꢄ 2.1V  
S  
RDEꢔ ꢍ RA  
2.1 ꢐ RDEꢔ  
RA ꢄ  
ꢄ 26.4kΩ  
S  
A ꢐ VO ꢉ 2.1  
3.2.4. Current-Sensing Resistor for PFC  
FL6300A has pulse-by-pulse current limit function. It is  
typical to set the pulse-by-current limit level at 20~30%  
higher than the maximum inductor current:  
0.8  
RCSꢟ  
(30)  
IDSPKꢀ1 ꢍ ꢠMAꢡGꢒN  
where KMARGIN is the margin factor and 0.8V is the cycle-  
by-cycle current limit threshold.  
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
9
AN-9736  
APPLICATION NOTE  
Vo  
R
1 1  
VOCꢮ Vꢑꢙꢂ_Cꢮ  
ꢀVꢑꢙꢂ_Cꢮ Vꢰꢙꢈꢃ ꢍ  
ꢱꢀVꢑꢙꢂ_Cꢮ Vꢰꢙꢈdt  
(32)  
Do  
C1  
Rꢝ  
Rꢝ  
C2  
Vsen_CC  
where the Vsen_CV means the sensing output voltage from  
the output stage and is divided by R4 and R8 resistor.  
R1  
Sensing resistor R4 and its value directly effect the CC  
control block output.  
R2  
C1  
R4  
R3  
Normally, the CC block is more dominate than the CV  
block in steady state and the CV block acts as the Over-  
Voltage Protection (OVP) at transient or abnormal mode,  
such as no load condition.  
VOCC  
VRef  
CC Control Part  
C2  
R7  
R5  
R8  
The output signal of CC block is determined as:  
Vsen_CV  
R6  
VOCV  
V
V
1
V
V
VOCC ꢄ Rꢑꢙꢂ_CC ꢰꢙꢈꢃ ꢍ ꢱꢀ ꢑꢙꢂ_CC ꢰꢙꢈꢃ dt (33)  
CV Control Part  
VRef  
Rꢎ  
Rꢛ  
ꢟ  
Rꢎ  
Rꢛ  
Figure 16. Feedback Circuit for CC/CV  
Operation  
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
10  
AN-9736  
APPLICATION NOTE  
3.3. Schematic of the Evaluation Board  
5
1
6
10  
4
2
3
1
Figure 17. Evaluation Board Schematic  
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
11  
AN-9736  
APPLICATION NOTE  
3.4. Bill of Materials  
Item No.  
Part Reference  
Value  
Qty.  
Description (Manufacturer)  
1
2
3
4
U101  
U102  
Q101  
Q102  
FL6961  
FL6300A  
1
1
1
1
CRM PFC Controller (Fairchild Semiconductor)  
QR PWM Controller (Fairchild Semiconductor)  
600V/20A MOSFET (Fairchild Semiconductor)  
800V/8A MOSFET (Fairchild Semiconductor)  
FCPF20N60  
FQPF8N80  
Ultra-Fast Recovery Power Rectifier  
(Fairchild Semiconductor t)  
5
6
7
D201,D202  
D103  
FFPF20UP30DN  
EGP30J  
2
1
4
600V/3A Ultra-Fast Recovery Diode (Fairchild Semiconductor)  
1000V/1A Ultra-Fast Recovery Diode  
(Fairchild Semiconductor)  
D104,D106,D107,D108  
RS1M  
8
D101  
Q201  
U202  
U203  
U201  
ZD103  
ZD201  
KBL06  
MMBT2222A  
LM2904  
FOD817  
KA431S  
24B 1W  
15B  
1
1
1
1
1
1
1
Bridge Diode (Fairchild Product)  
General-Purpose Transistor (Fairchild Semiconductor)  
Dual Op Amp (Fairchild Semiconductor)  
Opto-Coupler (Fairchild Semiconductor)  
Shunt Rregulator (Fairchild Semiconductor)  
Zener Diode (Fairchild Semiconductor)  
Zener Diode (Fairchild Semiconductor)  
9
10  
11  
12  
13  
14  
D102,D105,D203,D204,  
D205  
15  
LL4148  
5
General-Purpose Diode (Fairchild Semiconductor)  
16  
17  
18  
19  
20  
21  
22  
23  
24  
25  
26  
C101  
C102  
684/275V  
334/275V  
224/275V  
472(Y)  
1
1
1
2
1
3
4
3
1
1
2
X – Capacitor  
X – Capacitor  
C105  
X – Capacitor  
C103,C104  
C211  
Y – Capacitor  
222(Y)  
Y – Capacitor  
C106,C114,C206  
C107,C113,C116,C207  
C108,C109, C210  
C110  
33µF/50V  
104/2012  
105/2102  
68µF/450V  
222 1kV  
Electrolytic Capacitor, 105°C  
SMD Capacitor 2012  
SMD Capacitor 2012  
Electrolytic Capacitor, 105°C  
Ceramic-Capacitor  
SMD Capacitor 2012  
C111  
C112,C117  
200/2012  
C201,C202,C203,C204,  
C205  
27  
1000µF/35V  
5
Electrolytic Capacitor, 105°C  
28  
29  
30  
31  
32  
33  
34  
35  
36  
37  
38  
39  
40  
41  
42  
43  
C208,C209  
C212,C213  
F101  
474/2012  
102/3216  
220V/2A  
EI2820  
2
2
1
1
1
2
4
1
4
3
2
2
2
3
1
2
SMD Capacitor 2012  
SMD Capacitor 3216  
Fuse  
L101  
PFC Inductor (V10P), 450µH  
Stick Inductor  
L201  
10µH  
LF101,LF102  
R101,R102,R103,R104  
R128  
45mH  
Line Filter  
104/3216  
393/3216  
433/3216  
203/3216  
100/3216  
4R7/3216  
0R2 2W  
394/3216  
682/3216  
153/3216  
SMD Resistor 3216  
SMD Resistor 3216  
SMD Resistor 3216  
SMD Resistor 3216  
SMD Resistor 3216  
SMD Resistor 3216  
Metal Film Resistor 2W  
SMD Resistor 3216  
SMD Resistor 3216  
SMD Resistor 3216  
R105,R106,R107,R131  
R108,R124,R127  
R109,R118  
R110,R119  
R111,R122  
R112,R113,R114  
R115  
R213,R214  
44  
R116,R117  
2
Metal Oxide Film Resistor 2W  
150K/2W  
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
12  
AN-9736  
APPLICATION NOTE  
Bill Of Materials (Continued)  
Item No.  
Part Reference  
Value  
Qty.  
Description (Manufacturer)  
45  
46  
47  
48  
49  
50  
51  
52  
53  
54  
R120  
R123  
151/3216  
224/3216  
430/3216  
103/3216  
0.1/5W  
1
1
2
2
1
1
1
1
1
1
SMD Resistor 3216  
SMD Resistor 3216  
SMD Resistor 3216  
SMD Resistor 3216  
MPR Resistor 5W  
SMD Resistor 2012  
SMD Resistor 2012  
SMD Resistor 2012  
SMD Resistor 2012  
SMD Resistor 2012  
R125,R126  
R129,R130  
R201  
R202  
152/2012  
513/2012  
753/2012  
392/2012  
133/2012  
R203  
R204  
R205  
R206  
55  
56  
57  
58  
59  
60  
61  
62  
63  
R207,R209  
R208  
473/2012  
302/2012  
432/2012  
153/2012  
223/2012  
20k  
2
1
1
1
1
1
2
1
1
SMD Resistor 2012  
SMD Resistor 2012  
SMD Resistor 2012  
SMD Resistor 2012  
SMD Resistor 2012  
Variable Resistor  
NTC  
R212  
R210  
R216  
R211  
RT1,RT2  
T2  
5D-9  
EER3124  
10D471  
QR Transformer(V10P), 500µH  
VARISTOR  
RV1  
4.0 Related Datasheets  
FL6961 - Single Stage Flyback and Boundary Mode PFC Controller for Lighting –  
FL6300A -Quasi-Resonant Current Mode PWM Controller for Lighting  
Application Note - AN-6300 FAN6300/A/H - Highly Integrated Quasi-Resonant PWM Controller  
Application Note - AN-6961- Critical Conduction Mode PFC Controller  
DISCLAIMER  
FAIRCHILD SEMICONDUCTOR RESERVES THE RIGHT TO MAKE CHANGES WITHOUT FURTHER NOTICE TO ANY PRODUCTS  
HEREIN TO IMPROVE RELIABILITY, FUNCTION, OR DESIGN. FAIRCHILD DOES NOT ASSUME ANY LIABILITY ARISING OUT OF THE  
APPLICATION OR USE OF ANY PRODUCT OR CIRCUIT DESCRIBED HEREIN; NEITHER DOES IT CONVEY ANY LICENSE UNDER ITS  
PATENT RIGHTS, NOR THE RIGHTS OF OTHERS.  
LIFE SUPPORT POLICY  
FAIRCHILD’S PRODUCTS ARE NOT AUTHORIZED FOR USE AS CRITICAL COMPONENTS IN LIFE SUPPORT DEVICES OR SYSTEMS  
WITHOUT THE EXPRESS WRITTEN APPROVAL OF THE PRESIDENT OF FAIRCHILD SEMICONDUCTOR CORPORATION.  
As used herein:  
1. Life support devices or systems are devices or systems which,  
(a) are intended for surgical implant into the body, or (b)  
support or sustain life, or (c) whose failure to perform when  
properly used in accordance with instructions for use provided  
in the labeling, can be reasonably expected to result in  
significant injury to the user.  
2. A critical component is any component of a life support device  
or system whose failure to perform can be reasonably  
expected to cause the failure of the life support device or  
system, or to affect its safety or effectiveness.  
© 2011 Fairchild Semiconductor Corporation  
Rev. 1.0.0 • 4/8/11  
www.fairchildsemi.com  
13  

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