AND8331D [ONSEMI]

Quasi-Resonant Current- Mode Controller for High- Power ac-dc Adapters; 准谐振电流 - \n对于高模式控制器\n电源AC-DC适配器
AND8331D
型号: AND8331D
厂家: ONSEMI    ONSEMI
描述:

Quasi-Resonant Current- Mode Controller for High- Power ac-dc Adapters
准谐振电流 - \n对于高模式控制器\n电源AC-DC适配器

控制器
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AND8331/D  
Quasi-Resonant Current-  
Mode Controller for High-  
Power ac-dc Adapters  
Prepared by: Stéphanie Conseil  
ON Semiconductor  
http://onsemi.com  
Introduction  
Pin Description  
This document describes the implementation of the  
DAP013 inside an AC-DC adapter.  
Over Power Protection pin (OPP, pin 1): applying a  
negative voltage on this pin reduces the internal maximum  
peak current set point.  
Over Temperature Protection pin (OTP, pin 2): Connect  
an NTC between this pin and ground. An internal current  
source biases the NTC. When the NTC pulls the pin down,  
the circuit permanently latches-off.  
The DAP013 offers everything to build high performance  
AC-DC converters or offline adapters. Thanks to a novel  
valley lockout system, the controller is able to switch inside  
the drain-source valley and is immune to valley jumping  
instabilities. When the output load decreases significantly,  
the controller toggles to a fixed peak current/variable  
frequency mode that ensures very low standby power  
consumption. And last, but not least, the DAP013 features  
the usual protections that help to build cheap and safe power  
supplies: OVP, OTP, Brown-Out (C and D options),  
Short-circuit protection (latched for A, C versions and  
auto-recovery for D, F versions), soft-start, OPP, internal  
TSD...  
Timer pin (Timer, pin 3): Wiring a capacitor from this pin  
to ground helps selecting the timer duration.  
Zero Voltage Detection pin (ZCD, pin 4): Connected to  
the auxiliary winding, this pin detects the core reset event.  
Timing Capacitor pin (Ct, pin 5): A capacitor connected  
to this pin acts as the timing capacitor in VCO mode.  
Feedback pin (FB, pin 6): Hooking an optocoupler  
collector to this pin will allow regulation.  
To summarise, the DAP013 offers the following  
characteristics:  
Quasi-resonant Peak Current-mode Control Operation  
Valley Switching Operation with Valley-lockout for  
Noise-immune Operation  
Current Sense pin (CS, pin 7): This pin monitors the  
primary current and triggers the fault if needed.  
Ground pin (GND, pin 8): The controller ground.  
Driver pin (DRV, pin 9): This pin delivers pulses to the  
power MOSFET.  
Power Supply pin (V , pin 10): This pin supplies the  
CC  
VCO Mode (fixed peak current, variable frequency) in  
Light Output Load for Improved Standby Dissipation  
Internal 5 ms Soft-start  
controller and accepts voltage up to 28 V.  
Brown-Out pin (BO, pin 11): Allows shutting-down the  
controller for a chosen input voltage level. (C and D versions  
only)  
Over Voltage Protection pin (OVP, pin 12): By pulling  
this pin high, the controller can be permanently latched-off.  
High Voltage pin (HV, pin 14): Connected to the bulk  
capacitor, this pin powers the internal current source to  
Loss-free Adjustable Over Power Protection  
Auto-recovery or Latched Internal Output Short-circuit  
Protection  
Adjustable Timer for Improved Short-circuit Protection  
Over-voltage and Over-temperature Protection Inputs  
Brown-out Input for C and D Versions  
deliver a start-up current that charges the V capacitor.  
CC  
+500 mA / –800 mA Peak Current Source/Sink  
I. Over Power Protection  
Capability  
1. How Does It Work?  
Internal Temperature Shutdown  
Direct Optocoupler Connection  
3 ms Blanking Delay to Ignore Leakage Ringing at  
Turn-off  
Extremely Low No-load Standby Power  
SO14 Package  
A flyback operated in Quasi Resonant mode exhibits wide  
peak current variations in relationship to the input voltage  
conditions. As a result, the converter output power range  
widens as the input voltage increases. To cope with safety  
requirements, the designer needs to make the power output  
capability independent from the input conditions. A possible  
© Semiconductor Components Industries, LLC, 2008  
1
Publication Order Number:  
June, 2008 Rev. 0  
AND8331/D  
AND8331/D  
way of doing it is call Over Power Protection (OPP). The  
By applying this voltage through a resistor divider on the  
OPP pin, we have an image of the input voltage transferred  
to the controller via this pin. This voltage is added internally  
to the 0.8 V reference and affects the maximum peak current  
(see Figure 1). As the OPP voltage is negative, an increase  
of input voltage implies a decrease of the maximum peak  
current setpoint:  
novel technique implemented in the DAP00X takes benefits  
of the auxiliary winding voltage whose negative amplitude  
relates to the input rail voltage. When the power MOSFET  
is conducting, the auxiliary winding voltage becomes the  
input voltage V affected by the auxiliary to primary turn ratio  
IN  
Naux  
Np  
ǒN  
Ǔ:  
+
p,aux  
(eq. 2)  
VCS,max + 0.8 ) VOPP  
If OPP pin is grounded, there is no decrease of the peak  
current setpoint.  
Vaux + Np,auxVIN  
(eq. 1)  
R
R
upper  
CS  
+
OPP  
IpFlag  
-
+
Aux  
1
0.8 V + V  
opp  
ESD  
Protection  
+
lower  
0.8 V  
Figure 1. OPP Circuitry  
The amount of negative voltage that can be applied on the  
OPP pin is limited by the ESD diode placed on the pin to  
protect the silicon. Temperature characterization shows that  
But knowing the amount of current that will circulate  
inside the OPP diode for these values of V , it is possible  
OPP  
to set a higher bias current inside the resistor divider in order  
to neglect the diode leakage for OPP voltage lower than  
300 mV. Figure 2 shows the diode leakage at different  
this diode will start to conduct if the applied bias (V ) is  
OPP  
lower than 300 mV. Thus, if a voltage lower than 300 mV  
is applied on the OPP pin, the peak current decrease will no  
longer be linear.  
junction temperatures according to V . In any case, it is  
OPP  
forbidden to inject current higher than 2 mA in this pin  
otherwise, substrate injections could occur, leading to a  
possible erratic behaviour.  
100  
90  
80  
70  
125°C  
60  
50  
40  
30  
20  
10  
0
110°C  
25°C  
0.20  
0.25  
0.30  
0.35  
0.40  
0.45  
(V)  
0.50  
0.55  
0.60  
0.65  
V
OPP  
Figure 2. OPP Diode Leakage Current vs. VOPP at TJ = 255C, 1105C, 1255C  
In order to filter the switching noise on OPP signal, the designer can add a small capacitor between OPP and GND. This  
capacitor value can be adjusted according to the power MOSFET on-time duration at high line and must not be higher than 200 pF.  
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2. OPP Resistors Calculation  
Let us assume the design needs a peak current reduction of 34% at 370 V dc, therefore, the amount of voltage we must apply  
on pin 2 is:  
VOPP + 0.8   0.34 + 272 mV  
(eq. 3)  
By using the resistor divider law on R  
, R  
we obtain:  
upper lower  
Rlower  
Rupper * Rlower  
VOPP + *  
Np,auxVIN  
(eq. 4)  
Or:  
Rupper  
Np,aux  
V
IN * VOPP  
+ *  
(eq. 5)  
(eq. 6)  
Rlower  
VOPP  
If our auxiliary to primary turn ratio is 0.12, we obtain:  
Rupper  
Rlower  
0.12   370 * (0.272)  
0.272  
+ *  
[ 164  
Thus, we can select:  
= 160 kW and R  
R
= 1 kW  
lower  
upper  
The bridge current during the on time is:  
VOPP  
Rlower  
Ibridge  
Ibridge  
+
+
(eq. 7)  
(eq. 8)  
0.272  
1000  
+ 272 mA  
3. Why is the OPP Non Dissipative?  
Let us try to calculate the average current in the OPP bridge:  
Tsw  
Vaux(t)  
Rupper ) Rlower  
1
Tsw  
(eq. 9)  
ŕ
Ť
Ťdt  
Ibridge,mean  
+
0
After some calculations, we obtain:  
T
Ton  
off (VCC  
Tsw  
1
ǒ
) V )Ǔ  
(eq. 10)  
Ibridge,mean  
+
Np,auxVIN )  
f
Rupper ) Rlower Tsw  
Keeping up with our example from before, we can measure T , T , T on our adapter at 370 V dc, light output load (we  
on off sw  
are in VCO mode): T = 1.2 ms, T = 3.6 ms, T = 40 ms  
on  
off  
sw  
1.2 m  
160 k ) 1 k 40 m  
3.6 m  
40 m  
1
ǒ
25.6Ǔ+ 2.26 mA  
(eq. 11)  
Ibridge,mean  
+
  0.12   370 )  
If we had selected R  
= 100 W and R  
= 16 kW (meaning we impose a higher bias current in the resistor bridge), we  
lower  
upper  
would have I  
= 22.6 mA only!  
bridge  
4. OPP Trick  
From our previous example, we have calculated the OPP resistors in order to have a peak current reduction of 34% at 370 V  
dc that corresponds to V = -272 mV.  
OPP  
We obtained: R  
= 1 kW and R  
= 160 kW  
lower  
upper  
Now, with these resistors what will be the peak current reduction at 110 V dc?  
Rlower  
Rupper ) Rlower  
1
161  
VOPP + −  
Naux,pVIN  
+
  0.12   110 + 82 mV  
(eq. 12)  
This corresponds to a peak current reduction of 10.2% at low line. However because of the internal propagation delay, the  
peak current reduction is smaller is reality.  
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I
pk  
Set Point  
I
pk  
Set Point  
100%  
90%  
100%  
90%  
66%  
66%  
110  
220  
370  
110  
370  
V
IN  
(V)  
V
IN  
(V)  
Figure 5. Ipk Set Point over Input Voltage using a  
Zener in Series with the OPP Resistors  
Figure 3. Peak Current Set Point over the Input  
Voltage with Rupper = 160 kW and Rlower = 1 kW  
Design Example:  
We want to start reducing the maximum peak current  
around 220 V dc (roughly 155 Vrms).  
If we want to avoid losing 10% maximum of peak current  
at low line, we can introduce a simple threshold in the OPP  
circuitry through a zener diode placed in series with the  
resistive divider as shown in Figure 4.  
This extra diode allows selecting the input voltage at  
which we want to start applying over power compensation.  
This corresponds to an auxiliary winding voltage:  
(eq. 13)  
Vaux + Np,auxVIN + 0.12   220 + 26.4 V  
So we need a zener diode with a breakdown voltage:  
BVDZ + 0.12   (370 * 220) + 18 V  
(eq. 14)  
The new values for OPP resistors can be calculated using  
Equation 15:  
Zener  
Rupper  
Rlower  
Np,aux  
V
IN * BVDZ * VOPP  
(eq. 15)  
+ *  
OPP  
R
upper  
VOPP  
Aux  
Rupper  
Rlower  
0.12   370 * 18 * (0.272)  
0.272  
R
(eq. 16)  
+ *  
+ 98  
R
lower  
bias  
Cdec  
We choose: R  
= 100 kW and R  
= 1 kW  
upper  
lower  
II. Over Temperature Protection  
Figure 4. OPP with Zener Diode  
The adapter operating in a confined area, e.g. the plastic  
case protecting the converter, it is important to look after the  
internal ambient temperature. If this temperature would  
increase beyond a certain point, catastrophic failures could  
occur through semiconductors thermal runaway or  
transformer saturation. To prevent this from happening, the  
DAP00X embeds a novel Over Temperature Protection  
(OTP) circuitry appearing in Figure 6.  
V
DD  
OVP Comp  
20 ms Filter  
End of  
Softstart  
Ilatch  
2
-
+
OTP  
Cfilt  
+
VOTP  
NTC  
Figure 6. OTP Schematic  
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The I  
current (91 mA typ.) biases the Negative  
During start-up and soft-start, the output of the OTP  
comparator is masked to allow the voltage on pin OTP to  
grow if a filtering capacitor is installed across the NTC.  
The filtering capacitor value should be 1 nF.  
latch  
Temperature Coefficient sensor (NTC), naturally imposing  
a dc voltage on the OTP pin. When the temperature  
increases, the NTC’s resistance reduces (at 110°C, R  
=
NTC  
8.8 kW instead of 470 kW at 25°C) bringing the pin 2 voltage  
down until it reaches a typical value of 0.8 V: the comparator  
trips and latches-off the controller (Figure 7). Controller  
In DAP013, the OTP trip point corresponds to a resistance of:  
VOTP  
0.8  
RNTC  
+
+
+ 8.79 kW  
(eq. 17)  
Ilatch  
91 m  
reset occurs when a) the V is cycled from on to off b) the  
CC  
brown-out pin senses a stop condition on the bulk voltage.  
This corresponds to a temperature of 110°C using the  
TTC03-474.  
VCC  
VDRV  
VOTP  
Figure 7. Capture of an OTP Event. Here, the NTC was Heated with a Hairdryer...  
III. Timer Pin and Fault Management  
Protection against short-circuit or overload is insured by  
monitoring the current sense signal. The controller reaction  
is thus fully independent from the auxiliary to power  
comes back within safe limits, the “Max Ip” comparator  
becomes silent and the PWM comparator triggers the  
discharge of the timer capacitor. The timer capacitor is thus  
winding coupling. When the primary current exceeds I  
,
discharged by a constant current I . The internal  
timerD  
Limit  
the “Max Ip” comparator trips and the timer capacitor  
charges by the I current source. When the current  
circuitry appears in Figure 8.  
timerC  
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AND8331/D  
HV  
Vcc  
Vcc Management  
S
R
Vdd  
Q
Q
DRV  
Fault  
I
I
timerC  
PNOK  
PWM  
Reset  
Timer  
PWM  
Comparator  
+
CS  
-
+
C
timer  
timerD  
-
+
FB/4  
R
S
Vtim Fault  
Q
Q
Max Ip  
Comparator  
IpFlag  
+
OPP  
-
+
Ilimit + Vopp  
+
I
limit  
Figure 8. Timer Circuitry  
For D and F versions, when the voltage of timer capacitor reaches V , the output pulses are stopped and the controller  
timFault  
tries to re-start via a triple hiccup. (see Figure 9): this is the so-called auto-recovery operation.  
VCC  
Vdrain  
4.5 s  
Vtimer  
93 ms  
Figure 9. The Triple Hiccup in Fault Mode  
The triple hiccup helps to reduce the power consumption  
in fault mode. In Figure 9, the burst is only 2% for a 60 W  
For versions A and C, when V  
controller stops pulsing and stays latched. To reset the  
controller, the user must unplug the power supply to allow  
reaches V  
, the  
timer  
timFault  
adapter (with C  
= 100 mF).  
Vcc  
V
CC  
to drop below V  
level (5.5 V). (see Figure 10)  
CCreset  
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VCC  
VDRV  
5 V fault threshold  
VTimer  
Figure 10. The Latched Short-circuit Protection in A and C Versions  
Choosing Timer Duration and Timer Capacitor  
Where :  
While choosing the timer duration, the user must ensure  
that it is long enough to allow the power supply to enter  
regulation at low line and full load. (see Figure 11)  
The timer capacitor value can be calculated with:  
T  
is the duration before the fault validation  
is the charging current (10 mA typ. from  
fault  
I  
timerC  
datasheet)  
V  
is the timer voltage threshold at which the  
timFault  
fault is validated (5 V typ. from datasheet)  
Tfault timerC  
VtimFault  
I
Ctimer  
+
(eq. 18)  
VtimFault = 5 V  
VFB  
1 V  
Soft­start  
Vtimer  
VOUT  
Vdrain  
Figure 11. Timer Margin at Low Line, Full Load on a 19 V / 3 A Adapter  
IV. Zero Voltage Crossing Detection  
The Zero Crossing Detection circuit (ZCD) allows turning  
on the power MOSFET when the drain-source voltage is the  
lowest. This detection is achieved by monitoring the auxiliary  
winding voltage. The typical detection level is around 50 mV  
(Figure 12). By delaying this signal thanks to an RC network  
(the internal ESD protection features a parasitic capacitance  
of 10 pF) it is possible to switch right in the valley of the  
drain-source voltage.  
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AND8331/D  
VZCD  
V
Th  
Figure 12. Typical ZCD Signal. Here, the Power  
Supply Operates in 2nd Valley  
ZCD  
Rdem  
Resd  
+
-
demag  
+
Vth  
Aux  
Cdem  
Dz  
ESD  
Tblank  
GND  
DRV  
Leakage Blanking  
Figure 13. Zero Voltage Crossing Detection Circuit  
R
should be calculated to limit the current inside pin  
V. VCO Mode and Timing Capacitor  
1. How Does it Work?  
dem  
4 to less than +3 mA/-2 mA.  
For example, if the voltage on auxiliary winding is –45 V  
At nominal power, the power supply operates in a variable  
frequency system where discrete frequency steps occur as  
the controller looks for the different valley positions. At low  
output power, the controller enters a Voltage-Controlled  
Oscillator (VCO) mode where the switching frequency is  
at highest line, R  
22.5 kW.  
In order to avoid false triggering by the leakage  
inductance, a blanking circuit masks the ZCD signal during  
2 to 4 ms. So when designing the power supply, the designer  
must ensure that during valley operation, the  
demagnetization duration is higher than 4 ms. If not, the 1  
valley will also be blanked and valley switching instabilities  
will occur.  
should be higher than 45/0.002 =  
dem  
folded back. This mode is entered when V drops below  
FB  
0.8 V. The controller remains in this mode until V  
st  
FB  
increases above 1.4 V. During the VCO operation (V  
<
FB  
0.8 V), the peak current is frozen to 25% of its maximum  
value and the frequency diminishes as the output power  
decreases. (Figure 14)  
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Figure 14. Idrain, Vdrain, VCt, at Different Output Loads in VCO Mode  
The switching frequency is set by the end of charge of the  
timing capacitor C . This capacitor is charged by a constant  
0 V and a new period starts. The relationship between FB  
voltage and the internal threshold is:  
t
current source I and its voltage V is compared to an  
Ct  
Ct  
VFBth + 6.5 * (10ń3)VFB + VCt  
(eq. 19)  
internal threshold fixed by the FB loop. When V reaches  
Ct  
the threshold, the capacitor is rapidly discharged down to  
V
DD  
VCO  
Rpullup  
FB  
V
FBth  
6.5 (10/3) Vfb  
-
+
V
DD  
DRV  
S
R
Q
Q
ICt  
Ct  
Ct Discharge  
CS Comparator  
Figure 15. VCO Schematic  
th  
2. How to Calculate the Timing Capacitor Value?  
the switching frequency in the 4 valley and the switching  
The timing capacitor must be selected with care. Indeed,  
when the controller leaves the valley switching mode to  
enter the VCO mode, the frequency changes from a  
valley-position-controlled value to a switching frequency  
frequency imposed by the C capacitor, the frequency jump  
t
may create an instability by forcing the peak current to leave  
th  
its frozen state: an hesitation between 4 valley and the  
VCO mode takes place (Figure 16) and can create output  
ripple and noise.  
imposed by the C capacitor. If a too big gap exists between  
t
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th  
Figure 17 shows a normal transition from 4 valley to the  
VCO mode. At the beginning, the output load is such that it  
th  
imposes a V near 0.8 V in 4 valley operation, with a  
VFB  
FB  
switching period T . Then, if the load is slightly  
sw1  
Vdrain  
decreased, the FB voltage also passes below the 0.8 V  
threshold: the VCO mode is entered and the switching  
frequency decreases. (In VCO mode, the switching  
frequency is imposed by the FB voltage regardless of the  
position in the drain signal). The controller will stay in VCO  
mode until the FB voltage increases above 1.4 V. If we have  
an optimum timing capacitor value, the new steady state  
point is such that V is near 1.4 V and imposes a switching  
FB  
period T larger than T  
.
sw2  
sw1  
th  
VCO mode  
4
valley  
Figure 16. The Controller Hesitates between VCO  
Mode and 4th Valley: Ct is Too Big!  
Load  
V
FB  
1.4 V  
0.8 V  
V
FBth  
T
sw2  
T
sw1  
4th Valley  
VCO Mode  
Figure 17. 4th Valley to VCO Mode Transition with an Optimum Timing Capacitor Ct  
th  
To calculate C , we first need to estimate the switching period at the end of the 4 valley operation, for a FB voltage near  
t
0.8 V by using Equation 20 or by directly measuring it on our adapter:  
Nps  
0.2  
Rsense  
1
) 7p Ǹ  
Tsw1  
+
Lp  
ǒ
)
Ǔ
LpClump  
(eq. 20)  
VIN,minDC Vout ) Vf  
Where:  
R  
N = N /N is the primary to secondary turn ratio of  
ps s p  
is the sense resistor  
the transformer  
V is the output voltage  
sense  
0.2 relates to the voltage setpoint on the current-sense  
comparator when V = 0.8 V.  
out  
V is the output diode forward voltage  
FB  
f
L is the primary inductance  
C  
regroups all capacitances surrounding the drain  
p
lump  
V  
is the minimum DC input voltage, bulk  
node (MOSFET capacitor, transformer parasitics...). As  
a first approximation, you can use the MOSFET  
IN,minDC  
ripple included  
drain-source capacitance C  
instead of C  
.
OSS  
lump  
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Based on lab experiments, the switching period gap  
Thus, we can deduce the timing capacitor value knowing  
V , T and the charging current source I (20 mA typ.  
Ct sw2 Ct  
th  
between the end of 4 valley operation (T ) and VCO  
sw1  
mode (T ) for a FB voltage near 1.4 V (which is the  
from datasheet):  
sw2  
th  
threshold for VCO mode to 4 valley transition, V  
FB  
ICtTsw2  
1.83  
Ct +  
(eq. 23)  
increasing ) must not exceed 12 ms. Thus, for V = 1.4 V,  
we will have:  
FB  
Application Example: 19 V/60 W Adapter  
Tsw2 + Tsw1 ) 12 ms  
(eq. 21)  
V  
= 100 V  
V + V = 19 + 0.6 V  
IN,minDC  
Equation 13 allows calculating V for V = 1.4 V:  
Ct  
FB  
out  
f
VCt + 6.5 * (10ń3)   1.4 + 1.83 V  
(eq. 22)  
L = 190 mH  
p
C  
= 200 pF  
lump  
N = 0.25  
ps  
R  
= 0.25  
sense  
First, with Equation 14, we estimate T  
which is the  
sw1  
switching period of our power supply for an output load  
corresponding to a V = 0.8 V:  
FB  
Nps  
0.2  
1
) 7p Ǹ  
Tsw1  
+
+
LP  
ǒ
)
Ǔ
0.25  
LpClump  
(eq. 24)  
Rsense  
VIN,minDC Vout ) Vf  
0.2  
1
Ǹ
190   10*6  
)
  200   10*12 + 7.75 ms (129 kHz)  
*6  
ǒ100 19 ) 0.6Ǔ) 7p 190   10  
0.25  
When measured on the adapter we have: T = 8.47 ms (F  
= 118 kHz) corresponds to an ouput power of 9 W.  
sw1  
sw1  
We calculate the timing capacitor value:  
20   10*6(7.75   10*6 ) 12   10*6  
)
ICT(Tsw1 ) 12 m)  
(eq. 25)  
Ct +  
+
+ 216 pF  
1.83  
1.83  
We select C = 220 pF.  
t
VI. Feedback  
The feedback pin features an internal pull-up resistor  
which connects to the optocoupler, as shown in Figure 18.  
This pin is also connected to the internal valley comparators  
that will select the operating valley according to the FB  
voltage (see datasheet).  
It is recommended to add a capacitor between FB pin and  
GND pin of the controller. This capacitor has two  
advantages: it offers a filtering action on the FB signal and  
it forms with R  
a pole located at:  
pullup  
1
fp +  
(eq. 26)  
2p RpullupCpole  
This pole will help you to stabilize the power supply.  
Rpullup  
FB  
VII. VCC  
+
V
The DAP013 includes a high voltage startup circuitry that  
derives current from the bulk line to charge the V  
capacitor. When the power supply is first connected to the  
mains outlet, the internal current source is biased and  
DD  
5 V  
CC  
Cpole  
GND  
charges up the V capacitor. When the voltage on this V  
CC  
CC  
Figure 18. FB Pin Features an Internal Pull-up  
Resistor...  
The pull-up resistor value is typically around 20 kW and  
capacitor reaches the V  
level, the current source turns  
CCon  
off, reducing the amount of power being dissipated. At this  
time, the controller is only supplied by the V capacitor,  
CC  
is referenced in the datasheet.  
and the auxiliary supply should take over before V  
CC  
collapses below V  
. Figure 19 shows the internal  
CCmin  
arrangement of this structure:  
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11  
 
AND8331/D  
14  
Where:  
HV  
I  
is the controller consumption (see datasheet)  
CC2  
Q is the MOSFET total gate charge  
g
F is the switching frequency in maximum load,  
sw  
+
minimum input voltage  
IC1 or IC2  
-
Now, we need to estimate the total startup time.  
The high voltage startup circuit features two startup  
10  
8
+
levels, I and I . At power-up, as long as V is below  
C1  
C2  
CC  
V
(0.70 V typ.), the source delivers I (around 300 mA  
Th  
C1  
V
V
CCon  
+
typical). The duration is:  
CCmin  
VTh  
IC1  
t1 + CVcc  
(eq. 28)  
Then, when V reaches 0.70 V, the source smoothly  
CC  
transitions to I (6 mA typ.) and delivers its nominal value.  
C2  
When V reaches V  
, the source is turned-off:  
CC  
CCon  
Figure 19. Startup Circuitry  
1. How to Choose VCC Capacitor?  
VCCon * VTh  
t2 + CVcc  
(eq. 29)  
IC2  
The V capacitor is calculated to allow the power supply  
The total startup time is the sum of t , t and t  
.
CC  
1
2
reg  
to close the loop before V drops to V  
the time needed by the power supply to close the loop, the  
. If we call t  
CC  
CCmin  
reg  
VCCon * VTh  
VTh  
IC1  
ǒ
Ǔ
tstartup + CVcc  
)
) treg (eq. 30)  
IC2  
V
CC  
capacitor can be estimated with:  
(ICC2 ) QgFsw)treg  
VCCon * VCCmin  
For Example:  
CVcc  
+
(eq. 27)  
The time needed by the power supply to enter regulation  
is 45 ms worst case (full load).  
The MOSFET is a 6A / 600 V with a gate charge:  
Q = 24 nC  
g
(2.5   10*3 ) 24   10*9   65000) 45   10*3  
15 * 9  
(ICC2 ) QqFsw)treg  
VCCon * VCCmin  
(eq. 31)  
CVcc  
+
+
+ 30.45 mF  
We choose: C  
= 47 mF  
Vcc  
VCC  
IC2  
VOUT  
VTh  
IC1  
t1  
t2  
treg  
Figure 20. The Dual Level Startup Current Source in Action, Here with a Vcc Capacitor of 100 mF  
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12  
AND8331/D  
2. What is the Benefit of Using a Dual Level Startup Current Source?  
The dual level startup current source allows to limit the  
power dissipation of the controller in case of short-circuit  
to the highest T ), the device would dissipate 370 x 3 m =  
J
1.11 W.  
Thanks to the dual level startup, the current source deliver  
I = 300 mA if V is below 0.70 V. Thus, in case of  
C1  
between V and GND.  
CC  
Without the dual level startup, in high line conditions  
cc  
(V = 370 V dc), the current delivered by the startup device  
short-circuit between V and GND, the power dissipation  
HV  
CC  
will seriously increase the junction temperature. For  
will drop to 370 x 300u = 111 mW.  
instance, since I equals 3 mA (the minimum corresponds  
C2  
VIII. Brown Out  
The C and D versions of DAP013 feature a Brown Out pin  
(BO) which protects the power supply against low input  
voltage conditions (Figure 21). This pin permanently  
monitors a fraction of the bulk voltage through a voltage  
divider. When this image of bulk voltage is below the BO  
threshold, the controller stops switching. When the bulk  
voltage comes back within safe limits, the circuit goes  
through a new startup sequence including soft-start and  
re-starts switching (Figure 24). The hysteresis on brown-out  
pin is implemented with a low side current source sinking  
10 mA when the brown-out comparator is low (V  
<
bulk  
V
). This offers adequate precision at shutdown.  
bulk(ON)  
HVbulk  
+
VBO  
20 ms Noise Delay  
R
upper  
BO Reset  
BO  
11  
-
+
BO Comp  
R
lower  
IBO  
IBO “on” if BO Comp “low”  
IBO “off” if BO Comp “high”  
Figure 21. Brown-Out Circuit  
1. Calculating the BO Resistors  
V
V
bulk(ON)  
bulk(OFF)  
R
R
upper  
upper  
BO  
11  
BO  
11  
iu  
il  
iu  
ibo  
iu  
IBO  
R
R
lower  
lower  
Figure 22. Brown-out Equivalent Schematic at Startup  
Figure 23. Brown-out at Shutdown  
First of all, select the bulk voltage value at which the  
When V  
reaches V  
, the hysteresis current  
bulk  
bulk(ON)  
controller must start switching (V  
) and the bulk  
source is turned OFF. Thus, at shutdown, the BO voltage  
bulk(ON)  
voltage for shutdown (V  
we have:  
). According to Figure 22,  
only depends of V  
and R  
Rlower  
Rupper ) Rlower  
, R  
(Figure 23).  
bulk(OFF)  
bulk(OFF)  
upper lower  
VBO  
+
Vbulk(OFF)  
(eq. 34)  
iu + il ) IBO  
(eq. 32)  
Deducing R  
expression in Equation 33. We obtain:  
from Equatio 34, we replace R  
by its  
upper  
upper  
Where: I is the brown-out hysteresis current.  
BO  
By replacing i and i by their values, the previous  
u
l
V
BO(Vbulk(ON) * Vbulk(OFF))  
equation becomes:  
Rlower  
+
+
(eq. 35)  
(eq. 36)  
Vbulk(ON) * VBO  
IBO(Vbulk(OFF) * VBO)  
VBO  
Rlower  
+
) IBO  
(eq. 33)  
Rupper  
R
lower(Vbulk(OFF) * VBO  
)
Rupper  
VBO  
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13  
 
AND8331/D  
Design Example  
* VBO + 0.8 V  
V
BO(Vbulk(ON) * Vbulk(OFF)  
)
0.8(120 * 60)  
10 m(60 * 0.8)  
(eq. 37)  
(eq. 38)  
Rlower  
+
+
+
+ 81.1 kW  
* IBO + 10 mA  
IBO(Vbulk(OFF) * VBO  
)
* Vbulk(ON) + 120 V  
* Vbulk(OFF) + 60 V  
R
lower(Vbulk(OFF) * VBO  
)
81.1 k   (60 * 0.8)  
Rupper  
+
+ 6 MW  
0.8  
VBO  
VCC  
I
V
turns­on when  
is high enough  
BO  
CC  
VBO  
Vbulk  
BO threshold  
VDRV  
I
turns­off  
BO  
Figure 24. BO at Startup. The Controller Starts Pulsing if VBO > BO Threshold and VCC > VCCon  
IX. Over Voltage Protection  
The DAP013 also provides a protection against an over voltage condition (OVP), e.g. in case of the optocoupler destruction  
(Figure 25).  
VCC  
Vcc  
Ru  
Rl  
OVP  
12  
20 us filter  
+
or  
Rbias  
Vovp  
Figure 25. OVP Circuit  
The OVP pin (12) is connected to an internal comparator that will latch the controller if a voltage higher than 3 V is applied  
on this pin. Once the controller is latched, the user must unplug the power supply to allow V falling below V  
(around  
CC  
CCreset  
5 V) to reset the controller.  
As pin 12 is high impedance, the over voltage protection can be implemented also by using a resistor divider instead of the  
traditional zener diode.  
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14  
 
AND8331/D  
VCC  
VDRV  
OVP threshold  
VOVP  
Figure 26. Scope Shot of an Over voltage Event. Here, the OVP  
was Implemented with an 18 V Zener Diode  
X. Typical Application Schematic  
The schematic in Figure 27 shows the implementation of DAP013 inside a 19 V/60 W power supply.  
U4  
KBU4K  
C14  
100u  
L
D2  
MBR20200  
L3  
2.2u  
FL1  
Vout  
Gnd  
+
T1  
C1  
10n  
C9  
X2  
220nF  
IN  
C18  
100nF  
R4  
6.8k 6.8k  
D1  
R12  
N
C5a  
+
+
+
R1  
C7  
100uF  
25V  
C5b  
10  
R23  
6Meg  
1.2mF  
35V  
1.2mF  
35V  
1N4937  
R25, 6.8k  
U1  
DAP013D  
R18  
8.2k  
R30  
270k  
C15  
2.2nF  
C6  
22p  
Type = Y1  
Gnd  
R9  
1k  
14  
13  
12  
1
2
3
4
5
6
7
Lp = 190 mH  
Nps = 0.25  
Nauxp = 0.22  
D6  
1N967  
R22  
3Meg  
R5  
27k  
U5  
NTC  
R15  
1k  
R7  
U2a  
11  
10  
M1  
1N4937  
10  
C4  
330p  
D5  
R16  
SPP06N60  
9
8
39k  
R31  
1k  
C10  
47n  
C17  
1n  
D3  
R17  
22k  
R21  
82k  
R3  
U2b  
C5  
1n  
47k  
C13  
220n  
1N4148  
+
C20  
R29  
1k  
U3  
C11  
33u  
R8  
10k  
R26  
0.5  
R27  
0.5  
100n  
TL431  
C8  
220p  
Gnd  
Figure 27. 19 V /60 W Power Supply Schematic with DAP013D  
Conclusion  
This controller associate a quasi-resonant operation mode  
for high output loads with a VCO mode to improve the  
efficiency of the power supply at light loads.  
This application note has described in detail how to select  
the components surrounding the DAP013.  
The DAP013 contains all the features (OPP, OVP, OTP,  
short-circuit protection, BO...) to build high performance  
ac-dc power supplies.  
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15  
 
AND8331/D  
ON Semiconductor and  
are registered trademarks of Semiconductor Components Industries, LLC (SCILLC). SCILLC reserves the right to make changes without further notice  
to any products herein. SCILLC makes no warranty, representation or guarantee regarding the suitability of its products for any particular purpose, nor does SCILLC assume any liability  
arising out of the application or use of any product or circuit, and specifically disclaims any and all liability, including without limitation special, consequential or incidental damages.  
“Typical” parameters which may be provided in SCILLC data sheets and/or specifications can and do vary in different applications and actual performance may vary over time. All  
operating parameters, including “Typicals” must be validated for each customer application by customer’s technical experts. SCILLC does not convey any license under its patent rights  
nor the rights of others. SCILLC products are not designed, intended, or authorized for use as components in systems intended for surgical implant into the body, or other applications  
intended to support or sustain life, or for any other application in which the failure of the SCILLC product could create a situation where personal injury or death may occur. Should  
Buyer purchase or use SCILLC products for any such unintended or unauthorized application, Buyer shall indemnify and hold SCILLC and its officers, employees, subsidiaries, affiliates,  
and distributors harmless against all claims, costs, damages, and expenses, and reasonable attorney fees arising out of, directly or indirectly, any claim of personal injury or death  
associated with such unintended or unauthorized use, even if such claim alleges that SCILLC was negligent regarding the design or manufacture of the part. SCILLC is an Equal  
Opportunity/Affirmative Action Employer. This literature is subject to all applicable copyright laws and is not for resale in any manner.  
PUBLICATION ORDERING INFORMATION  
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