AN708 [VISHAY]

Low-Power Universal-Input Power Supply Achieves High Efficiency; 低功耗通用输入电源实现高效率
AN708
型号: AN708
厂家: VISHAY    VISHAY
描述:

Low-Power Universal-Input Power Supply Achieves High Efficiency
低功耗通用输入电源实现高效率

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AN708  
Vishay Siliconix  
Low-Power Universal-Input Power Supply  
Achieves High Efficiency  
Expanding global markets have created a demand for what  
secondary –– a figure that is totally inconsistent with the desire  
to achieve low leakage inductance. As a result, cross  
regulation between primary and secondary- referenced  
windings will be poor. This complicates the regulation of the  
have become known as universal-input power supplies –– that  
is, power supplies that allow devices to be plugged into wall  
outlets anywhere in the world. These power supplies must be  
able to operate directly from 100-, 110-, and 220-V ac power  
lines without the use of selector switches or jumpers. A power  
supply with the ability to operate under such conditions while  
remaining cost-effective is now becoming a necessity.  
primary-side  
bootstrap  
winding  
used  
to  
avoid  
secondary-to-primary feedback across the isolation boundary.  
The addition of a simple spike-blanking circuit solves the  
problem (see AN707, “Designing Low-Power Off-Line Flyback  
Converters Using the Si9120 Switchmode Controller IC”).  
In the under 30-W power range, meeting the above  
requirements while maintaining high efficiency has been a  
challenge. Add to this the need to meet various international  
safety standards, and the circuit designer has his hands full.  
When using the Si9120 for universal-input applications, it is  
recommended that a bootstrap winding be employed. While  
not strictly necessary, the power dissipation and chip  
temperature are higher if bootstrapping is not utilized. As an  
example, at VIN = 400 V dc and ICC = 1.5 mA, the power  
dissipation on the chip without a bootstrap is 600 mW. If a 10 V  
bootstrap supply is used, the dissipation is only 15 mW. This  
becomes more of a concern as the gate charge requirements  
of the power MOSFET increase, since the value of ICC for the  
controller is largely dependent on gate drive demands.  
The demands of low-power universal-input power suppliesare  
met by the Si9120 pulse width modulation (PWM) controller  
from Vishay Siliconix. Using the Si9120, the flyback circuit  
presented in this application note demonstrates that designing  
universal-input supplies can be a simple task.  
Another advantage of the DCM flyback converter is its  
single-pole loop response. This makes compensating the  
feedback loop comparatively simple. In addition, transient  
response can be quite good in DCM flyback converters. It is  
possible (though not practical in a closed-loop system) to slew  
the power stage from no load to full load in only one switching  
cycle.  
CIRCUIT TOPOLOGY  
For the low power levels that are of interest here (under 30 W),  
the discontinuous-mode (DCM) flyback converter is the  
preferred topology. The biggest advantage of this topology is  
simplicity. The parts count in the power path cannot get any  
lower.  
DESIGN EXAMPLE  
The peak-to-average primary current ratio in a DCM flyback is  
high relative to other topologies; however, at low power levels,  
this is not a serious drawback. On-state losses are minimal.  
Magnetics are small. Also, the transformer reset voltage is set  
by the minimum input voltage and remains fairly constant as  
thelinevoltagechanges. Asaresult, a600-VMOSFETproves  
adequate, even with ac inputs up to 300 V RMS.  
The circuit shown in Figure 1 is an 11.1-W, 3-output off-line  
supply. The input voltage is specified from 90- to 260-V ac.  
Outputs are +5 V at 1.5 A, +12 V at 150 mA, and –12 V at  
150 mA. The design features full VDE isolation, primary side  
regulation, and true foldback current limiting. Operating  
frequency is 100 kHz.  
The DCM flyback converter, when operated under  
current-mode control, provides a natural input volt-second  
limit, which helps keep the drain voltage from getting out of  
control during line or load transient conditions. Also, today’s  
power MOSFETs are able to withstand avalanche current  
many times greater than a low power circuit can typically  
deliver (see appendix A). As such, the MOSFET will serve as  
a clamp for the occasional spike which may result from a short  
circuit or extreme load transient.  
DCM flyback operating principles are generally well  
understood and will not be presented here. Refer to  
Vishay Siliconix Application Note AN707 for a detailed design  
example. References 2 and 3 are also recommended.  
Sizing the input capacitor and rectifiers for universal input  
requires more thought than for comparable single-input  
converters. Keepinmindthatwhilethemaximuminputvoltage  
occurs at high-input line, the maximum current stresses will  
occur at low line. This implies that the input capacitor value  
must be sized at low line while the voltage rating is dictated by  
the high-line condition. The bridge rectifier should be rated at  
600-V dc minimum. The RMS current rating is calculated  
below.  
Cross regulation is fairly good, especially if leakage  
inductance between windings can be kept low.[1] In a  
universal-input application, meeting VDE input-to-output  
isolation requirements is essential. Depending on the end  
product, this can be as high as 3750-V RMS, primary to  
Document Number: 70581  
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AN708  
Vishay Siliconix  
L1  
D3  
DB105  
ac In  
C18  
C17  
0.1 mF  
X
90 – 260 V ac  
0.1 mF  
50/60 Hz  
X
8 mH  
+
C8  
0.0047 mF  
450 V  
C7  
33 mF  
450 V  
+12 V, 150 mA  
D7  
T1  
C19  
0.0047 mF  
C20  
0.0047 mF  
MUR110  
C21  
2200 mF  
C22  
0.47 mF  
+
Y
Y
16 V  
50 V  
RTN  
RTN  
R16  
10 kW  
C6  
1000 pF  
D1  
R2  
175 kW  
MUR110  
C4  
2200 mF  
C5  
0.47 mF  
+
U1  
1
8
9
7
16 V  
50 V  
D8  
5
4
OUT  
16  
12  
BIAS  
SD  
R4  
10 W  
Q1  
SMP4N60  
–12 V, 150 mA  
Si9120  
SENSE  
R3  
1 kW  
13  
11  
6
10  
14  
15  
C10  
0.1 mF  
50 V  
C15  
N/U  
R5  
1.3 W  
C11  
4700 pF  
R14  
390 kW  
R9  
2 kW  
C6  
1000 pF  
100 V  
R1  
10 W  
C12  
1000 pF  
100 V  
L2  
6 mH  
R6  
20 W/W  
+5 V, 1.5 A  
D2  
D5  
D4  
C1  
2200 mF  
6.3 V  
C2  
1000 mF  
6.3 V  
C3  
0.1 mF  
50 V  
1N4148  
D6  
1N4148  
1N5822  
+
+
R13  
75 kW  
R12  
8.2 kW  
R10  
130 kW  
1N4148  
RTN  
C9  
220 pF  
R7  
1.2 kW  
C14  
1 mF  
50 V  
Q3  
2N4403  
C13  
4700 pF  
Q2  
2N7000  
R15  
40.2 kW  
R11  
68 kW  
R8  
680 W  
FIGURE 1. Schematic for Universal-Input Power Supply  
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AN708  
Vishay Siliconix  
For the present example:  
choosing an operating frequency and calculating the peak  
primary current, a value for primary inductance, LP, can be  
determined as follows:  
Output power = 5.0 V x 1.5 A + 12 V x 0.15 A x 2 = 11.1 W  
If efficiency is assumed to be 70%,  
Input power = 11.1 W/0.7 = 15.86 W  
For 100 kHz, period = 10 ms.  
At 50% duty factor, ton(max) = 5 ms.  
For a little cushion, assume a low-input line voltage of 85 V ac.  
I
pk  
= I x 4  
in  
= (0.1586 A) (4)  
= 0.634 A pk.  
Thus,  
Ǹ
V
dc + 85 2 + 120V dc.  
For VIN (dc) = 100 V  
dt  
L + V  
Ipk  
Assuming a 20-V pk-pk input-capacitor ripple voltage the  
minimum voltage is  
(
) (  
0.634 A  
)
100 V 5E–6 s  
V
= 120 V – 20 V = 100 V.  
min  
+
I
in  
= P /V  
in DC  
= 788 mH.  
= 15.86 W/ 100 V = 0.1586 A  
dt  
The actual inductance used was 735 mH. [For high-volume  
production applications, the design engineer should consider  
the worst case tolerances for clock frequency and inductor  
value.]  
C + I  
dv  
0.1586 A x 0.01 s  
20 V  
+
= 79 mF  
See AN707 for transformer design equations and a fully  
worked example.  
68 mF is a standard value. With 68 mF, the ripple voltage is  
dt  
C
V
pp + I  
The biggest considerations for universal input are related to  
the additional insulation required to comply with VDE isolation  
specifications. The physical space occupied by the insulation  
typically reduces the useable fill factor to 25%. Furthermore,  
the increase in leakage inductance caused by large physical  
separation of the windings has the undesirable effects of  
creating large voltage spikes on the power MOSFET drain,  
contributing to power losses, and degrading load regulation.  
0.16 A   0.01 s  
+
68E–6F  
= 23.5 V, an acceptable value.  
The capacitor voltage rating is calculated:  
Ǹ
V
max + 260 V ac x 2 + 368 V dc.  
Barrier tape at window ends will take up a lot of useable space,  
so a core geometry with a long, low window should be selected  
to minimize wasted area. This has the added benefit of  
reducing leakage inductance. (See equation 6.4 of  
reference 4.)  
A 400-V capacitor is acceptable. A rating of 450-V dc is  
preferable if high reliability is required or significant line  
transients are expected.  
Assuming a power factor of 0.65, the RMS input current is  
Po  
Wind the primary first. Apply the required insulation, and then  
wind the secondaries. All secondaries should be wound  
together with no intervening insulation, if voltage levels allow.  
Optimal cross regulation is achieved in this way.  
Iac  
+
hac (PF)  
11.1 W  
) ( ) (  
0.7 85 V 0.65  
+
(
)
= 0.287 A  
Further reductions in leakage inductance can be realized by  
using interleaved windings. First wind one half of the primary,  
followed by the secondaries and remaining primary turns. The  
multiple primaries are usually connected in parallel. The spike  
blanking circuit described in AN707 virtually eliminates the  
primary-to-secondary leakage inductance problems, at least  
from the standpoint of the regulation effects.  
A 1-A bridge rectifier is more than adequate.  
The primary inductance value is chosen by analyzing the  
lowest input voltage case. For a given load, the value of the  
peak transformer primary current will remain constant  
regardless of the input voltage. Since the primary inductance  
is fixed, the time to ramp to a given value of current is inversely  
proportional to input voltage (V = Ldi/dt). Therefore, low line is  
where the most time is needed to ramp to the desired primary  
current. The duty factor limit dictates an on-time limit. After  
In selecting a power MOSFET, the main concerns will be the  
r
DS(on) and the drain voltage ratings. The transformer primary  
voltage during the off time is VP = (Vo + VD) NP/NS. Using the  
5-V winding,  
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V
= (5.0 V + 0.4 V)(45 T/3 T) = 81  
keeps C13 charged to VCC. Hence, Q3 is biased off. In the  
event of a short circuit on any output, all winding voltages are  
clamped low. This causes the voltage on C13 to drop to a level  
setbydividerR10andR11. VCC isheldat8.6VbytheSi9120’s  
start-up regulator. The current set by the value of R12 flows  
through Q3 and R3, and causes the voltage on pin 4 to rise.  
Since a peak threshold of 1.2 V is internally set on pin 4, the  
voltage required across R5 to terminate a pulse is reduced by  
an amount equal to the drop on R3.  
P
Therefore,  
V
DS(off)  
= V  
+ V = 368 V + 81 V = 449 V.  
IN(max) P  
A 600 V MOSFET allows for a 150 V spike due to leakage  
inductance at high line. The RC snubber was sized empirically  
to keep the peak drain voltage below 600 V.  
The SMP4N60 is the smallest 600-V device available. At 25_C  
the rDS(on) is 2.0 W. At 100_C, rDS(on) = 1.75 x 2 W = 3.5 W. The  
peak drain current was previously calculated at 0.634 A. The  
maximum RMS drain current is given by  
I
D
= {1.2 - (I )(R3)}/R5.  
Q3  
Thus as IQ3 increases, ID decreases.  
See Figure 2a for foldback operating waveforms.  
1
2
0.5  
3
D
Ǹ
ǒ Ǔ  
+ 0.634A ǒ Ǔ+ 0.26 A  
IRMS + Ipk  
3
The foldback circuit will not perform correctly without the spike  
blanking circuit. The leakage spike will peak charge C13 even  
with a shorted load. However, the foldback function is  
completely optional and all associated components can be  
eliminated if a lower cost supply is desired.  
On-state losses are given by  
2
P
on  
= I  
x r  
DS(on)  
RMS  
2
= (0.26 A) x 3.5 W  
= 237 mW.  
TEST RESULTS  
Switching losses are estimated at 350 mW. Since the thermal  
resistance is specified at 80_C/W, a total temperature rise of  
47_C is expected. This permits operation up to approximately  
50_C ambient temperature, while holding the maximum  
junction temperature to 100_C.  
Data compiled on the test circuit appear in Table 1. Combined  
line and load regulation measures "2.7%, well within a "5%  
specification. Measured efficiency is 73.4% with no effort at  
optimization.Adetailedlossassessmentcould, nodoubt, offer  
some improvements. Pulse load tests show reasonable  
transient response, and phase margin is measured at  
60 degrees. For details on how to close the feedback loop,  
refer to Vishay Siliconix application notes AN713 and AN707.  
Something of more concern for universal-input than for a  
single-input voltage supply is the range of duty factor to be  
expected. Sincetheontimevariesinverselywithinputvoltage,  
the high-line on-time can become quite small in  
a
high-frequency converter. For this kind of application, try to  
keep the minimum on time to not much less than 1 ms. This will  
help minimize noise problems with the current sense.  
All data taken with dc input source to ensure stable readings.  
TABLE 1. UNIVERSALĆINPUT SUPPLY  
TEST DATA  
Also, be sure to use a non-inductive resistor for the current  
sense (carbon composition or film type). Use of a wire-wound  
resistor will produce large spikes which have to be filtered out.  
The dual-delay current-limit comparators of the Si9120 will  
frequently eliminate the need for a current-sense filter  
altogether. The magnitude of the noise on the current sense  
voltage will be affected by transformer parasitic capacitances  
and PCB layout. As such, every design will exhibit slightly  
different characteristics. Careful attention to detail in the  
magnetics design and construction as well as the board layout  
is a must.  
Full Load:  
VIN (dc)  
Iin (mA)  
+5 V  
+12 V  
–12 V  
100 V  
200 V  
300 V  
385 V  
143.9  
72.3  
48.9  
39.4  
4.974  
5.014  
5.027  
5.049  
12.64  
12.76  
12.79  
12.81  
12.50  
12.61  
12.65  
12.67  
Half Load:  
100 V  
200 V  
300 V  
385 V  
78.0  
40.3  
27.9  
23.0  
5.153  
5.205  
5.235  
5.254  
12.99  
13.10  
13.12  
13.14  
12.83  
12.96  
12.97  
13.01  
For designs using current-sense resistors in the power  
MOSFET’ssourceleg,notethatthegatedrivecurrentisseen”  
by the sense resistor. In very low-power designs, this can  
easily exceed the full load sense voltage causing severe noise  
problems. Adding a fairly large-value gate resistor will help in  
this case. Also, an RC current-sense filter becomes much  
more important.  
PKĆPK OUTPUT RIPPLE VOLTAGES  
(SPIKES NOT INCLUDED)  
5 V  
+12 V  
45 mV  
–12 V  
FOLDBACK CIRCUIT  
60 mV  
40 mV  
Foldback current limiting is provided by Q3 and its associated  
components. Under normal operating conditions, diode D6  
Note: Worst case over full line-voltage range.  
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a)  
Short Circuit On 5 V Output  
Q1 Drain Voltage (100 V/Div)  
Voltage On U1, Pin 4 (Current Sense)  
(0.5 V/Div)  
NOTE: 0.8 V dc pedestal caused by  
the foldback circuit.  
b)  
Q1 Drain Voltage (100 V/Div)  
Q1 Gate Voltage (100 V/Div)  
c)  
Q1 Gate Drive (5 V/Div)  
Voltage On U1, Pin 4 (Current Sense)  
(0.5 V/Div)  
FIGURE 2. Operating Waveforms (all photos full load, V = 150 V dc)  
IN  
Measured efficiency at VIN = 300 VDC was 73.4%.  
good example of where trade-offs can be made during  
development programs. By using the larger input capacitance  
and primary inductance, the peak input current could be  
reduced slightly, and a slight improvement in efficiency should  
result. However, a larger input capacitance will decrease the  
conduction angle of the input rectifiers, and consequently will  
reduce the input power factor. The priorities of a particular  
application will determine the optimal approach.  
During testing, an input capacitor value of as little as 33 mF  
proved adequate versus the design value of 68 mF. The  
low-value capacitor produces an input ripple voltage of 30 V  
pk-pk. Since the primary inductance is slightly lower than the  
design maximum value, the circuit is still able to maintain  
regulation with the higher input ripple voltage value. This is a  
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Vishay Siliconix  
V
CC to Rbias and typical Ibias. The equation given can be used  
CONCLUSION  
for points not on the graph.  
The simple universal-input power supply design that has been  
presented combines economy and performance which should  
prove more than adequate for the majority of applications. The  
overallcostofthesupplyshouldrivallinearregulatorsofsimilar  
power level if heatsink cost is considered. Good regulation has  
been achieved while maintaining the 3750-V ac  
input-to-output isolation mandated by VDE. The Si9120  
eliminates the need for any external start-up circuitry. Also,  
foldback current-limiting is demonstrated which requires no  
feedback across the isolation boundary.  
14.0  
13.0  
12.0  
11.0  
10.0  
9.0  
APPENDIX  
A
The SMP4N60 was tested for ability to withstand repetitive  
avalanche currents and for non-repetitive capability.  
Inductance values of 12 mH and 94 mH were used. Repetitive  
tests were run at 3 A, with 94 mH at 25_C. Failure current was  
measured at 25_C and 100_C. Results were as follows:  
8.0  
5
15  
25  
35  
45  
mA  
55  
65  
75  
85  
Ǹ
VCC – 2.3 V – 484 Ibias  
Rbias  
+
Ibias  
L
=
9mH4  
L
=
1mH2  
25_C  
4.25 A  
100_C  
2.40 A  
25_C  
7.28 A  
100_C  
6.40 A  
FIGURE 3. Relationship of V to R  
an Typical I  
CC  
bias  
bias  
REFERENCES  
For the 11.1-W flyback supply presented here, the leakage  
inductance is specified at 60 mH maximum. The maximum  
drain current is set to approximately 1.0 A. Therefore, based  
on the above data, adequate margin is present to prevent  
avalanche failure.  
1) Liu, K.H., “Effects of Leakage Inductance on the Cross  
Regulation in a Discontinuous-Mode Flyback Converter,”  
Proceedings, 1989 High Frequency Power Conference,  
Naples, Florida.  
2) Chryssis, G., “High Frequency Switching Power Supplies,”  
McGraw Hill 1984.  
APPENDIX  
B
A number of performance parameters of the Si9120 can be  
alteredbysettingIbias to a value other that 15 mA. AtlowerIbias  
higher efficiency can be obtained. At higher Ibias, lower  
propagation delays and a wider error amplifier bandwidth are  
possible. Also, if a VCC supply other than 10 V is used, Rbias  
shouldbesomethingotherthan 390 kW.Figure3belowrelates  
,
3) Billings, K., “Switchmode Power Supply Handbook,”  
McGraw Hill 1989.  
4) McLyman, Col. W.T., “Transformer and Inductor Design  
Handbook,” McGraw Hill 1988.  
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UNIVERSAL INPUT POWER SUPPLY PARTS LIST  
C1 . . . . . . . . . . . . . 2200 mF, 6.3 V Al. Electrolytic – United Chemicon SXC  
C2 . . . . . . . . . . . . . 1000 mF, 6.3 V Al. Electrolytic – United Chemicon SXC  
C3, C10 . . . . . . . . . 0.1 mF, 50 V Ceramic, Vishay Vitramon VJ1206Y104KXAAT  
C4, C21 . . . . . . . . . 2200 mF, 16 V Al. Electrolytic – United Chemicon SXC  
C5, C22 . . . . . . . . . 0.47 mF, 50 V Ceramic, Vishay Vitramon VJ1210Y474KXAAT  
C6, C12 . . . . . . . . . 1000 pF, 100 V Ceramic. Vishay Vitramon VJ1206Y102KXBAT  
C7 . . . . . . . . . . . . . 33 mF, 450 V Al Electrolytic (400 V ok)  
C9 . . . . . . . . . . . . . 220 pF, 100 V Ceramic, Vishay Vitramon VJ1206A221KXBAT  
C11, C13 . . . . . . . . 4700 pF, 100 V Ceramic, Vishay Vitramon VJ1206Y472KXBAT  
C14 . . . . . . . . . . . . 1 mF, 50 V Ceramic, Vishay Vitramon VJ1812Y105KXAAT  
C16 . . . . . . . . . . . . 75 pF, 500 V Ceramic or Mica, Vishay Vitramon VJ1206A750KXEAT  
C17, C18 . . . . . . . . 0.1 mF, 250 V,ac VDE Class X2 Wima MKS 4-R, Vishay Roederstein F17724102000  
C8, C19, C20 . . . . 0.0047 mF, 250 V,ac VDE Class Y Wima MP3-Y, Vishay Roederstein F17724102000  
D1, D7 . . . . . . . . . . MUR 110 Motorola 1 A 100 V  
D2 . . . . . . . . . . . . . 1N5822 3 A, 40 V Schottky  
D3 . . . . . . . . . . . . . Bridge 1 A, 600 V DB105  
D4, D5, D6 . . . . . . 1N4148  
L1 . . . . . . . . . . . . . . Common mode choke Renco 1361-2  
L2 . . . . . . . . . . . . . . Inductor 6 mH, 1.5 A, Vishay Dale ILS-1206-6 mH "10%  
Q1 . . . . . . . . . . . . . FET N-channel SMP4N60 Vishay Siliconix  
Q2 . . . . . . . . . . . . . FET N-channel 2N7000 Vishay Siliconix  
Q3 . . . . . . . . . . . . . 2N4403 PNP (or 2N2907)  
R1, R4 . . . . . . . . . . 10 W, 1/8 Carbon Film or Metal Film, Vishay Dale TNPW120610R0FT2  
R2 . . . . . . . . . . . . . 175 kW, 1/8 W Carbon Film or Metal Film, Vishay Dale TNPW12061753FT2  
R3 . . . . . . . . . . . . . 1 kW, 1/8 W Carbon Film or Metal Film, Vishay Dale TNPW12061001FT2  
R5 . . . . . . . . . . . . . 1.3 W, 1/4 W Metal Film  
R6 . . . . . . . . . . . . . 20 W, 1/2 W Metal Film  
R7 . . . . . . . . . . . . . 1.2 kW, 1/8 W Metal Film, Vishay Dale TNPW12061201FT2  
R8 . . . . . . . . . . . . . 680 W, 1/8 W Metal Film, Vishay Dale TNPW12066800FT2  
R9 . . . . . . . . . . . . . 2 kW, 1/8 W Metal Film, Vishay Dale TNPW12062001FT2  
R10 . . . . . . . . . . . . 130 kW, 1/8 W Metal Film, Vishay Dale TNPW12061303FT2  
R11 . . . . . . . . . . . . . 68 kW, 1/8 W Metal Film, Vishay Dale TNPW12066802FT2  
R12 . . . . . . . . . . . . 8.2 kW, 1/8 W Metal Film, Vishay Dale TNPW12068201FT2  
R13 . . . . . . . . . . . . 75 kW, 1/8 W 1% Metal Film, Vishay Dale TNPW12067502FT2  
R14 . . . . . . . . . . . . 390 kW, 1/8 W Metal Film, Vishay Dale TNPW12063903FT2  
R15 . . . . . . . . . . . . 40.2 kW, 1/8 W 1% Metal Film, Vishay Dale TNPW12064022FT2  
R16 . . . . . . . . . . . . 330 W, 1/2 W 5% Carbon Composition  
T1 . . . . . . . . . . . . . . Schott Corp. #67122700  
Document Number: 70581  
www.vishay.com S FaxBack 408-970-5600  
7
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Datasheets for electronics components.  

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