Implementing a Medium Power AC-DC Converter with the NCP1395

AND8257/D
Implementing a Medium
Power AC−DC Converter
with the NCP1395
Prepared by: Roman Stuler
ON Semiconductor
http://onsemi.com
APPLICATION NOTE
INTRODUCTION
during the light load conditions. Standby consumption of
whole supply can thus be significantly decreased.
This document describes all the necessary design steps
that need to be evaluated when designing the NCP1395
controller in an LLC resonant converter topology. A 240 W
AC−DC converter has been selected for the typical
application.
The design requirements for our 240 W AC−DC
converter example are as follows:
Requirement
Min
Max
Unit
Input Voltage
90
265
Vac
Output Voltage
−
24
Vdc
Output Power
0
240
W
Operating Frequency
65
125
kHz
Efficiency Under Full Load
90
−
%
No Load Consumption
−
1000
mW
Timer Based Fault Protection
The converter stops operation after a programmed delay
when this input is activated. This protection can be
implemented as a cumulative or integrating characteristic.
Thus under transient load conditions the converter output
will not be turned off, unless the extreme load condition
exceeds the timeout.
Internal Transconductance Amplifier
This internal transconductance amplifier can be used to
create effective overload protection. As the result the power
supply can be operated in either CV or CC mode. This
feature is very useful for the battery chargers applications.
Common Collector Optocoupler Connection
The open collector output allows multiple inputs to the
feedback pin, for example overcurrent sensing circuit,
overtemperature sensor, etc. The additional input can pull up
the feedback voltage level and take over the voltage
feedback loop.
Please refer to the NCP1395A/B data sheet for a detailed
description of all the functions.
LLC series resonant converter topology has been selected
to meet efficiency requirements. The NCP1395 resonant
mode controller is a very attractive solution for such designs
because it offers the following features.
Brownout Protection Input
Demo Board Connection Description
The schematic for the 240 W demo board is shown in
Figure 1. The demo board contains three blocks: a PFC front
stage (which is necessary for the required power level and
to restrict the bulk voltage operating range of the
downstream resonant converter), an LLC converter, and an
auxiliary buck converter which provides bias power for PFC
and LLC controllers.
The NCP1653A PFC controller is used to control the PFC
front stage. Capacitors C1−C5 together with BALUNs L1, L2
and varistor VDR1 forms the EMI filter which suppresses
noise conducted to the mains.
The divided down input voltage of the converter is
permanently monitored by the Brownout pin (pin name). If
the voltage on the bulk capacitor falls outside of the desired
operating range, the controller drive output will be shut off.
This feature is necessary for an LLC topology because it is
usually optimized to operate over a narrow range of bulk
voltages.
Immediately Fault Input
This input can be used as a shutdown input in some
applications (LCD television SMPS, etc.). It can also be
used to induce skip mode operation of the LLC converter,
© Semiconductor Components Industries, LLC, 2006
September, 2006 − Rev. 2
1
Publication Order Number:
AND8257/D
AND8257/D
E11
+
R45
R46
220 m/63 V
R40
R39
C24
D13
NU
1000 m/35 V
1000 m/35 V
C23 NU
33 n
NU
D7
NU
1000 m/35 V
D15B
D8
MBRF20100CT MBRF20100CT
TR1
R34
100 mH
R36
1k2
STP12NM50FP
R37
M2
R32
IC5
PC817C
NU
C22
220 p
L4
1m5
15 V
E3
2u2/450 V D1
R27
5k6
220 k
R25
C21 10 n
0R
R23
R30
C7
C6
NINV
330 n
R1
0.1R
R9
330 n
11 k
R5
2M2
R7
R6 470 k
CV275K10B1
2n2/Y1
2n2/Y1
Rt
56 k
NCP1653
R8 3k3
KBU810
R22
IC1
C17
C9
1n
C12
C13
39 n
1n
C14
100 n
C4
3k3
L2
C3
470 n
C2 NU
3m3
L1
C1
470 n
Figure 1. Schematic of the NCP1395 Demo Board
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2
R21
C16
150 k
4u7
NU
C15
1u
R18
R17
100 k
NU
N
AC INPUT
90−265 VAC
L
T3, 15 A
100 n
330 k
680 k
F1
3m3
C18
R20
R19
RTH1 NU
2M2
C5
IC2
100 n
VCC
10 k
NCP1395
DRV
Gnd
VDD
4R7
VDR1
4n7
R12
C11
R11
1N5408
B1
100 n
R16
R10
L3
650 mH
56 k
C20 1 n
+
E12 NU
2k7
Voff
IN
C
D6
D5
MURA160
R15
D2 470 k 750 k 750 k
CSD0660A
SPA20N60C3
M1
PC817
+
R14
FB
C8 1 n
1M2
NU
C19
C10
Gnd
Drain IC3
FB
IC4
R47
300 k 470 k 470 k
+
E2 150u/450 V
+
E1 150u/450 V
R2
R3 R4
D3
E4
VCC
2k2
PGnd
D4
R13
1 k 47 m
+
MURA160
NCP1012AP065
220 m/25 V
+
E5
R33
33 k
NU
7V5
10 k
MURA160
4M7
D12
D16
10 k
G_HI
S_HI G_LO S_LO
GND
VCC
DRIVER MODULE
DRV_LO
DRV_HI
R48
AGnd
R31
2n2/Y1
R26
BC846BLT1 R29
Q1
R24
180
NU
C25
B
A
L5
STP12N
M50FP
M3
R35
IC6
TL431 C28
1k
R28
100 R
D11
NU
C26
R38
NU
D10
D9
3k3
BO
D14B D15A
TR2
CST1−100LB−
COILCRAFT
R41
2k7
22 n
VCC
D14A
1000 m/35 V
1000 m/35 V
R42
FB
Ctimer
E6
R44
1k
OUT
S.F.
F.F.
E7
C290 1 n
Fmax
DT
CSS
E10
E9
E8
+
+
+
+
+
5k6
NU
18 k
L6
2.2 mH
R43
C27
NU
PE
AND8257/D
A bridge rectifier is used to rectify the input AC line
voltage. Capacitors C6 and C7 filter the high frequency
ripple current, which is generated by the PFC stage. In this
application a Classical PFC boost topology is used. The PFC
power stage is formed by: inductor L3, MOSFET switch M1,
SiC diode D2, bulk capacitors E1, E2 and inrush current
bypassing diode D1. The current in the PFC stage is
monitored by current sense network R1, R8//R9. The output
voltage of the PFC stage is regulated to a nominal 400 Vdc
via feedback loop components R2−R4 and C9. Part of the
rectified input voltage is taken by the divider R5−R7 and
capacitors C13, C14 to create over power protection of the
PFC switch. Capacitor C12 filters the control voltage and
sets the PFC feedback loop bandwidth. Devices connected
to Pin 5 of the NCP1653A set the operation mode of the PFC
stage to CCM and also dictate over power protection level.
Please refer to the application note AND8184/D for detailed
explanation how to design a PFC using the NCP1653A
controller.
An ON Semiconductor NCP1012 monolithic switcher is
used for the auxiliary buck converter. This converter
provides a stable Vcc to assures proper operation of the PFC
and LCC controller under all operating conditions and fault
conditions, such as when a short−circuit is applied to the
output of the LLC converter.
The NCP1012 is connected as a high side switch. Diode
D3 is the freewheeling diode. The input power for the buck
converter is supplied from the rectified mains via diode D5
and electrolytic capacitor E3. Feedback is done via diode D6,
optocoupler IC4 and capacitor C8. Supply voltage of the
NCP1012 is maintained on the capacitor E4 using diode D4,
resistor R13 and internal DSS architecture. The internal
dynamic self supply block is inactive during steady state
operation decreasing the power consumption of the buck
converter. The output voltage of the buck converter is
regulated to 16 V allowing some margin above the PFC
controller VccON level, which is 15 V maximum. Please
refer to application note AND8191/D for other information
regarding NCP10xx products.
As it was previously mentioned the NCP1395 resonant
mode SMPS controller is used to control the LLC converter
power stage, provide output voltage regulation, and fault
protection.
The power stage of the LLC converter is formed by bulk
capacitors E1, E2, MOSFETs M2, M3, resonant inductor L5,
transformer TR1 and resonant capacitor C23. A center
tapped winding is used on the secondary side to increase
efficiency of the converter. Electrolytic capacitors E6−E11
together with inductor L6 serve as an output filter.
The output voltage is set at 24 Vdc using a TL431 (IC6)
for feedback. The resistive divider formed by R46, R42 and
R43 provide a sample of the output voltage to the reference
pin of the TL431 (2.5 V). The control loop feedback
compensation is done with the series combination of
capacitor C26 and resistor R41. The biasing current for the
IC6 is provided by the resistor R44. The optocoupler IC
current is set by the series resistor R40.
The current through the feedback optocoupler is
translated to a voltage on the primary side by the resistor R33.
The voltage is then applied to the NCP1395 feedback pin. A
Zener diode, D12, clamps the maximum feedback voltage
and resistor R28 limits the current through D12.
The output power level at which the controller enters skip
mode is set by the voltage divider R26, R27. The fast fault
input is filtered by the capacitor C20. Resistor R30 sets the
voltage gain on the output of the operational
transconductance amplifier, capacitor C21 is used for the
current feedback loop compensation. The voltage on the
OTA output is clamped to 7.5 V maximum with the resistor
R47 and Zener diode D16. The clamp is necessary because a
higher voltage could cause the controller to enter skip mode
during startup, or during overload. The output current level
for which the skip mode takes place (during the overload
conditions) is set by the divider R24, R25.
The primary current for the LLC power stage is sensed by
current transformer TR2 along with diodes D8−D11,
resistors R35, R36, and capacitor C22. An alternative to the
current transformer is to sense the primary current with the
sensing circuit formed by the resistors R38, R39 diodes D7,
D13 and capacitor C24. This alternative is included in the
demo board layout.
The minimum operating frequency of the converter is set
by the resistor R18, and the maximum operating frequency
is set by resistor R19. The dead time between the outputs A
and B is set by the resistor R20. The soft−start duration is set
by capacitor C15, and the timer duration is set by capacitor
C16 together with resistor R21.
The Brown Out circuit monitors the bulk capacitor
voltage with the resistive divider set by R14, R15, R16, R22,
and capacitor C18. When the bulk capacitor voltage drops
outside the desired operating range of the LCC converter, the
output drives are turned off.
A decoupling capacitor, C19, is used between the ground
and Vcc pin of the controller to improve the noise immunity.
The switches for the Half Bridge (M2 and M3) are driven
from a High Side Driver module which is mounted vertically
on the converter’s main board. This arrangement allows the
designer to test the entire driver topology quickly and easily.
Two versions of the driver are available as demo board
accessories. Schematics for both versions are shown in
Figures 2 and 3. One version uses the NCP5181 − integrated
high voltage driver and is tailored for consumer applications
where the price is important.
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3
AND8257/D
R6
22R
D9
G−Hi
Q1
BC817−40LT1
MMSD4148
R7
10R
+Vcc
T1
D1
Input A
R3
10k
R1
150R
D2
C1
100 n
Q6
BC807−40LT1
D11
18 V
D10
MMSD4148
D12
18 V
Q2
BC807−40LT1
S−Hi
G−Lo
MMSD4148
D1−D4
Q3
BC817−40LT1 MBR140
R5
22R
R8
10R
D5
D3
Q5
BC807−40LT1
D7
18 V
D6
MMSD4148
D8
18 V
Input B
R4
10k
R2
150R
C2
100 n
D4
GND
S−Lo
Q4
BC807−40LT1
Figure 2. Connection of the MOSFET Driver with Transformer
D1
MURA160
R1
18R
R5
0R
Input A
IC1
IN_Hi
Input B
R4
0R
VBOOT
C1
100n
R2
10R
IN_Lo DRV−Hi
G−Hi
Bridge
S−Hi
GND
Vcc
CRV_LO
NCP5181
+Vcc
C2
100n
R3
10R
G−Lo
S−Lo
GND
Figure 3. Connection of the MOSFET Driver with NCP5181 −
Integrated Driver
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AND8257/D
• Same component count as half bridge topology: The
Design steps for resonant tank components values are
described in details below.
component count is nearly the same between an LLC
converter and a classical HB configuration.
LLC Converter Stage Design
An LLC resonant converter is an attractive topology in
comparison to a traditional half bridge for the following
reasons:
• An LCC converter is capable of ZVS while operating
over the entire set of anticipated load conditions.
With ZVS the switches are turned on when its drain
voltages are zero, the result is nearly zero turn−on
losses and a reduction in the EMI signature. The classic
half bridge topology, which uses hard switching, can
have significant turn−on switching losses and this can
increase the EMI signature.
• Low turn−off current: switches are turned off under low
current and thus the turn− off losses are also lowered in
comparison to a classical half bridge topology.
• Zero current turn−off of the secondary diodes: when the
converter is operating under full load condition, the
output rectifiers are turned of under zero current which
results in an reduced EMI signature.
Disadvantages of the LLC converter lie in these features:
• Higher peak and RMS currents in the primary and
secondary windings in comparison to the classical HB
topology. Thus this topology isn’t very attractive for
very high output current levels.
• Narrow input voltage operating range: LLC converter
has to be optimized for narrow input voltage range, if
one wants to take full advantage of the topologies
benefits.
• Changeable operating frequency: operating frequency
of the LLC converter has to vary to keep the output
regulated.
LLC Resonant Converter Operation Description
The LLC resonant converter power stage is shown in
Figure 4.
+
C1
M1
Control
Circuit
T1
D1
C2
LR
+
RL
LM
M2
CR
D2
Figure 4. Power Stage of the LLC Resonant Converter
One can observe three resonant components in this
topology: LR–resonant inductance, LM–magnetizing
inductance of the transformer and CR− resonant capacitor.
We can define two different resonant frequencies using
Thompson’s Equations 1 and 2:
fr1 +
fr2 +
1
2 · p · ǸLr · Cr
1
2·p·
Ǹ(Lr ) Lm) · Cr
This topology behaves like a frequency dependent divider
which is shown in the Figure 5 schematic.
CR
(eq. 1)
VIN
LR
LM
RAC
(eq. 2)
Figure 5. Substitutive Schematic
of the LLC Resonant Converter
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VOUT
AND8257/D
One can find the gain transfer function of the divider if the
fundamental analysis is used [4], [5]. The main idea of this
analysis is that only the fundamental frequency is passed
through the resonant tank. As a result of this simplification,
the real loading resistance needs to be converted to
equivalent loading resistance Rac using Equation 3.
Rac +
8 · RL
p2 · n2 · h
Three operating areas can be identified in these
characteristics:
1. In this area (above the resonant frequency fr1)
the converter works as series resonant converter.
The transformer magnetizing inductance never
participates on the resonance because it is clamped
by the converter output – one of the secondary
diode is conducting for entire switching period.
ZVS condition is naturally assured in this operation
area for the entire load.
2. In this area the LLC converter works like a multi
resonant converter. Let us go through one
switching cycle (please refer to the timing diagram
depicted in Figure 8).
(eq. 3)
Where:
RL is the real loading resistance
n is the transformer turns ratio
h is expected efficiency
Using an equivalent load resistance (Rac) we can calculate
the gain transfer characteristic of the LLC converter and
obtain the characteristic for any given value of load
resistance, resonant tank components, and quality factor of
the resonant circuit. The fastest way to do it is to use SPICE
simulator. The result of such simulation can be seen in
Figure 6.
Figure 8. Typical waveforms of the LLC converter
operating in the 2nd area of the gain
characteristic.
Figure 6. Typical Gain Characteristic of the LLC
Resonant Converter
The load will change in the real application so it is
necessary to plot the characteristic for several different load
conditions in one graph. We can use parametric analysis to
produce Figure 7.
One of the MOSFET switches is turned on. The resonant
inductance Lr resonates together with the resonant capacitor
Cr while the magnetizing inductance is clamped by the
converter output – one of the secondary diode is conducting.
When the resonant current decreases to a low value (the
same as the magnetizing current) the output diode stop
conducting and magnetizing inductance comes to play. The
resonant circuit has thus been reconfigured to Lr+Lm – Cr.
The resonant frequency fr2 is low in comparison to the
resonant frequency fr1. Thus the primary current slowly
increases. This current stores energy in the magnetic
components − mainly in the magnetizing inductance. Now
the switching cycle is forced (by the driver) to be finished.
The energy stored in the magnetic components causes ZVS
for the opposite MOSFET switch using its body diode.
3. In this area the converter entering to the zero
current switching mode. This could happen when
converter is overloaded. Some protection circuit
(passive or active) has to be implemented to
prevent entering this area.
Figure 7. Couple of Gain Characteristic for
Different Load Conditions
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AND8257/D
d) Minimum output current: 0 A – skip mode has to be
implemented to assure low power consumption under no
load.
e) Operating frequency limits: from 65 kHz to 125 kHz.
f) Converter should work under series resonant frequency
(fr1) for 400 VDC nominal input voltage and full loaded
output. This frequency should be below 100 kHz.
Based on the input requirement f) we can calculate turns
ratio of the LLC transformer. Voltages on the resonant
capacitor Cr and resonant inductor Lr are the same values but
opposite orientation when converter works at resonant
frequency fr1. Thus the gain of the converter is given only by
the transformer turns ratio value under this operating
condition (assume that the leakage inductance of the
transformer is low in comparison with magnetizing
inductance). We can calculate needed turns ratio value using
Equation 4:
The big advantage of the LLC series resonant converter is
the fact that the output can be regulated over the entire load
range, while the change of the operating frequency is not as
high as for other types of resonant converters.
Design of the resonant tank components i.e. Lr, Lm, and Cr
is always compromise between maximum load changes,
maximum acceptable operating frequency excursion, value
of the circulating energy in the resonant circuit and short
circuit characteristic. Behavior under short circuit is not an
issue when some overcurrent protection is used – like with
the NCP1395 controller.
The best way to operate an LLC resonant converter from
the efficiency and EMI point of view is to let it work directly
at the resonant frequency fr1. Under these conditions the
switching losses are minimized, circulating energy in the
resonant tank is also low and secondary diodes are turned off
under zero current so there are nearly no reverse recovery
losses. This optimal operating point can be reached only for
one given input voltage and load resistance value. Thus in
the practice the LLC converter is usually designed using
these operating conditions i.e. under series resonant
frequency fr1 for full load and nominal bulk voltage (which
is given by the PFC stage). When the load is decreased the
operating frequency is increased by the feedback loop to
keep the output voltage regulated. On the other hand
converter has also to cope with the bulk voltage drops, due
to transient loading (PFC regulation loop is very slow). Also
hold up time requirements come into play. The converter
will also operate under resonant frequency fr1 in these
special cases. The minimum operating bulk voltage of the
LLC converter can be effectively limited using the
NCP1395 Brown Out input pin.
One important thing that has to be taken into account
during the LLC designing is the fact that the manufacturing
tolerances of the inductors and capacitors are pretty high for
standard production. If one wants to have good repeatability
for resonant converter design then higher accuracy of these
components has to be specified or the LLC converter has to
be designed with higher margins.
n+
Np
Ns
+
Vin
400
+
[ 8 (eq. 4)
2 · (24 ) 0.8)
2 · (Vout ) Vf)
Where:
Np is the primary turns count
Ns is the secondary turns count
Vin is the input voltage (PFC output)
Vout is the wanted output voltage
Vf is the secondary diode voltage drop
ETD29 core has been selected for the transformer
construction. The primary turns count can be calculated
using Equation 5:
Np +
Vin
8 · DB max · fswmin · Ae
(eq. 5)
400
+
[ 40
8 · 0.25 · 65 · 103 · 76 · 10−6
where:
DBmax is the maximum flux density excursion
fswmin is the minimum operating frequency of the converter
Ae is the core effective area
The minimum switching frequency will be reached only
in special cases − overload and bulk voltage dropouts. The
flux density excursion will be always lower for normal
steady state operation mode – hysteresis losses.
The secondary turns count can be calculated using
Equation 6:
Transformer and Resonant Tank Components
Design
Based on the mentioned recommendations we can start
with the LLC resonant tank components design.
Input variables:
a) Input voltage range i.e. PFC output voltage:
350–420 VDC, 400 VDC nominal.
b) Output voltage: 24 VDC.
c) Max output current: 10 A continuous, overcurrent
protection with 115% threshold.
Np
Ns + n + 40 + 5
8
(eq. 6)
Needed copper area of the primary and secondary windings
can be calculated based on the RMS current values.
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AND8257/D
Now we can calculate resonant components values. There
are many variables that can be chosen by the designer,
however, poor choices can result in converter efficiency
degradation or too wide operating frequency range. It is
necessary to take the following into account, during the
design:
1. Quality factor of the resonant tank Q (and also its
characteristic impedance) will significantly affect
the gain characteristic and thus also the operating
frequency range. If the Q of the resonant circuit is
high, the gain characteristic will be narrow and the
operating frequency range will be low. However, if
the Q is too high the characteristic impedance will
be low and converter operation under overload
will be degraded.
2. The Lm/Lr = k ratio will also significantly
influence shape of the gain characteristics and thus
the ZVS region borders [5], [6].
Based on the previous simulations and calculations Q of
3 and k = Lm/Lr = 6 ratio have been chosen.
Now we can calculate characteristic impedance Z0 of the
resonant circuit using Equation 7:
Z0 +
2
n2 · RL
+ 8 · 2.4 + 51.2 [ 51 W
3
Q
Cr = 33 nF
fop = fr1 = 85.1 kHz
Now we can start simulation of the resonant converter to
obtain gain characteristic for full loaded converter.
Simulation schematic, which includes the leakage
inductance of the transformer, is depicted in Figure 9.
V1
1V
L4
R4
33 n
100 mH
0.1
TX1
R1
(Rac)
24 V
Output
0
0
Figure 9. Simulation Schematic of the
Proposed Converter
The gain values we are looking for can be calculated from
Equations 11 through 13:
(eq. 7)
The resonant capacitor value can be calculated from
Equation 8. Let us select the nominal operating frequency
fop = fr1 = 85 kHz for full load and nominal bulk voltage:
1
Cr +
2 · p · fr · Z0
1
+
+ 36.7 nF
2 · 3.14 · 85 · 103 · 51
Cs
(eq. 8)
G min +
2 · (Vout ) Vf)
2 · (24 ) 0.8)
+
+ 0.118 (eq. 11)
420
Vin max
Gnom +
2 · (Vout ) Vf)
2 · (24 ) 0.8)
+
+ 0.124 (eq. 12)
400
Vinnom
G max +
2 · (Vout ) Vf)
2 · (24 ) 0.8)
+
+ 0.142 (eq. 13)
350
Vin min
Operating frequencies for these gains can be read from the
simulated gain characteristic which is depicted in Figure 10.
An E6 standard value capacitor of 33 nF has been chosen.
The characteristic impedance will then change to 56.7 W and
Q will be 2.71.
Now we can easily calculate the resonant inductance
value, which is given by Equation 9:
Lr + Z02 · Cr + 56.72 · 33 · 10−9 + 106 mH
(eq. 9)
Use standard E6 value of Lr = 100 mH.
The magnetizing inductance is given by the selected k
ratio (Equation 10):
Lm + k · Lr + 6 · 100 · 10−6 + 600 mH (eq. 10)
Now we have nearly all needed for the simulation and
obtain gain characteristic. However, for accurate results the
leakage inductance of the transformer has to be taken into
account. This inductance will affect on the resonance and it
will also change gain of the converter somewhat. We have
selected the ETD29 transformer core with classical winding
technique so we can assume that the leakage inductance
will be around 1% of the magnetizing inductance i.e.
Llk = 6.0 mH. Let us now summarize real values of the
resonant tank components:
Figure 10. Simulated Gain Characteristic of
Proposed LLC Converter – Full Load Conditions
As can be seen the operating frequency range is 61 kHz to
101 kHz, for a fully loaded converter output and with the
input voltage range. The simulated operating frequency for
the nominal input voltage and full load current is 88 kHz,
which is very near to the calculated resonant frequency fr1.
One can see that there is enough gain margin to keep the
converter in the ZVS region (Region 2 in Figure 7) even
during a slight overload on the output.
Lr’ = Lr + Llk = 106 mH
Lm = 600 mH
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AND8257/D
0.95
0.93
When the load resistance is increased the gain of the
converter will increase too, because of the Q changes.
Moreover, the drops in the transformer copper and
secondary diodes are lower for lower loading current. For
these reasons the feedback loop will try to increase the
operating frequency to lower the converter gain. If
maximum operating frequency limit is set too low, the
feedback loop will not be able to regulate the output. This is
exactly what we need to assure skip mode for light load.
Under such conditions the feedback pin voltage goes up and
triggers the fast fault input via resistor divider R26, R27.
Simulation can again be used to find the maximum needed
frequency for light load regulation. If the maximum
operating frequency is limited to 125 kHz skip mode will be
automatically implemented.
Let us summarize the simulations and design results:
1. Converter should operate at fop [ fr1 = 88 kHz for
full load and nominal bulk voltage.
2. Operating frequency range is 61 kHz to 101 kHz,
at full load, over the input voltage range.
3. Operating frequency goes above fr1 frequency for
light loads.
4. For very light loads, the converter will reach the
maximum frequency limit and the feedback will
activate fast fault input. Skip mode will thus take
place.
Vin = 230 V/50 Hz
EFFICIENCY (%)
0.91
Vin = 110 V/60 Hz
0.89
0.87
0.85
0.83
0.81
0.79
0.77
0.75
1
2
3
4
5
6
7
8
9
10
Iout (Adc)
Figure 11. Efficiency of the Designed Converter
versus Output Current
EFFICIENCY (%)
0.93
0.92
0.91
0.90
Overcurrent Protection Circuitry
The Q of the resonant tank can drop to a very low value
during overload conditions. To overcome incorrect
operation in the ZCS region, the primary current has to be
limited by the overcurrent protection circuit. This circuit has
been already mentioned. The onboard OTA takes over and
pulls up the feedback pin via transistor Q1 when input
current goes over the desired maximum value.
0.89
90 110 130 150 170 190 210 230 250 270
Vsc in (Vrms)
Figure 12. Efficiency of the Example Converter
versus Input Voltage for Full Loaded Output
Results Summarization
Operating frequency of the real demo board prototype is
83 kHz for full load and 395 VDC input voltage which is
very close to the theoretical results.
Output current level for which the skip mode takes place
has been set to 400 mA using resistor divider R26, R27. Skip
level is given by the feedback voltage and thus it is very
sensitive to the resonant component values and output
voltage setup accuracy!
Measured efficiency for different input voltages and load
conditions can be seen in Figures 11 and 12.
Loading characteristic of the prototype can be seen in
Figure 13.
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OUTPUT VOLTAGE (Vdc)
25
20
15
10
5
0
1
2
3
4
5
6
7
8
9
10 11 12
OUTPUT CURRENT (Adc)
Figure 15. Detail of the ZVS Condition –
Rising Edge
Figure 13. Loading Characteristic of the Proposed
Converter
One can see that the CV operation is possible up to 10 A
load current. Then the overcurrent circuit starts to limit
output power and finally the hiccup mode takes place when
output current goes over 11.4 A.
Several snapshots taken from the prototype can be seen in
Figures 14 through 22.
Standby consumption is below 1.0 W for both input
voltage levels, i.e. 230 VAC and 110 VAC.
Figure 16. Detail of the ZVS Condition –
Falling Edge
Figure 14. Primary Current and Waveforms for Full
Loaded Converter
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Figure 17. Load Regulation for 230 V Input Voltage
Figure 20. Operating Under Short Circuit
Figure 18. Output Ripple Under Full Load
Figure 21. Full Load to Short Circuit Transition
Figure 19. Output Ripple During the Skip Mode
Figure 22. Operation in the Skip Mode
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Layout Consideration
Leakage inductance on the primary side is not very critical
for LLC converters compared to other topologies, because
it will only slightly modify the resonant frequency. However
it is well to keep the areas of each power loop as small as
possible due to radiated EMI noise. A two−sided PCB with
one side a ground plane helps (see Figures 23 through 26).
Special care has to be taken with Pins 1, 2 and 3 of the
NCP1395 controller because these are high impedance pins.
Ensure that these pins are not near high voltages and high
dV/dt or use some ground shielding.
Literature
1. NCP1395A/B data sheet.
2. Application note AND8184/D.
3. Application note AND8191/D.
4. Application note AND8255.
5. Bo Yang − Topology Investigation for Front End
DC−DC Power Conversion for Distributed Power
System.
6. Milan Jovanovich – Resonant converters training
brochure.
7. M. B. Borage, S. R. Tiwari and S. Kotaiah −
Design Optimization for an LCL – Type Series
Resonant Converter.
CAUTION
This board is intended only for demonstration and
evaluation purpose. Board is designed for free air
operation. Temperature damage of its components can
occur if the board will be placed under the cover without
forced air cooling.
Figure 23. Conducted EMI Signature of the Board
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Figure 24. Component Placement on the Top Side (Top View)
Figure 25. Top Side (Top View)
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Figure 26. Component Placement on the Bottom Side (Bottom View)
Figure 27. Bottom Side (Bottom View)
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Figure 28. Photo of the Designed Prototype (Real Dimensions are 183 x 122 mm)
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NCP1395 Demo Board Parts List
Designator
B1
C1,C3
Description
8.0 A Bridge Rectifier
EMI Suppression Capacitors (MKP)
C2
Value
Manufacturer Part Number
KBU810
KBU810
470n
B81130B1474M
NU
C4, C5
Safety Ceramic Disc Capacitor
2n2
KZH 2200PF M 2E3 500 Y1/X1 B1
C6,C7
Polyester Chip Capacitor
330n
R46X−0,33UF 15 275V M M1 00
C8, C9, C13
SMD Capacitor
1nF
VJ0806Y102KXBAx
C10
SMD Capacitor
4n7
VJ1206Y472KXBAx
C12
SMD Capacitor
39n
VJ0806Y393KXBAx
C14
SMD Capacitor
100n
VJ1206Y104KXBAx
C15
SMD Capacitor
1u
VJ1206Y105KXBAx
C16
SMD Capacitor
4u7
VJ1206Y475KXBAx
C17
NU
C11, C18, C19
SMD Capacitor
100n
VJ1206Y104KXBAx
C20, C29
SMD Capacitor
1n
VJ1206Y102KXBAx
C21
SMD Capacitor
10n
VJ1206Y103KXBAx
C22
SMD Capacitor
220p
VJ1206Y221KXBAx
C23
Polypropylene Capacitor
33n
R73−0,033UF 15 630V J 00 AA
C24
NU
C25
Capacitor, Y1 Class
C26
SMD Capacitor
2n2/Y1
WKP222
22n
VJ1206Y223KXBAx
C27
NU
C28
NU
D1
3.0 A 1000 V Standard Recovery Rectifier
D2
600 V; 4.0 A; Zero Recovery Rectifier
D3, D4, D5
D6
1N5408
1N5408
CSD04060A
CSD04060A
MURA160
MURA160
MMSZ15T1
MMSZ15T1
Surface Mount Ultrafast Power Rectifier
Zener Diode 500 mW 15 V
D7
D8, D9, D10,
D11
NU
Small Signal Switch Diode 100 V
MMSD4148T1
D12
NU
D13
NU
D14A,B;
D15A,B
D16
20 A 100 V Schottky Rectifier
Zener Diode 500 mW 7.0, 5.0 V
MMSD4148T1
MBRF20100CT
MBRF20100CT
MMSZ7V5T1
MMSZ7V5T1
E1,E2
Radial Lead Electrolytic Capacitor
150u/450V
K05 105°C 1500 mF/
450V 0514 13592
E3
Radial Lead Electrolytic Capacitor
2u2/450V
CERA−2,2/450 10x12,5 KMG
E4
Radial Lead Electrolytic Capacitor
47u/25V
CERA−47/25 5x11 CD268
E5
Radial Lead Electrolytic Capacitor
220u/25V
CERA−220/25 8x12 LXZ
E6, E7, E8, E9,
E10
Radial Lead Electrolytic Capacitor
1000u/35V
CERA−1000/35 12,5x25 LXZ
E11
Radial Lead Electrolytic Capacitor
220u/63V
CERA−220/63 10x16 A KMG
E12
NU
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NCP1395 Demo Board Parts List
Designator
Description
F1
Fuse
IC1
Compact Fixed−Frequency Current−Mode
PFC Controller
IC2
Resonant Mode SMPS Controller
IC3
Self−Supplied Monolithic Switcher for Low
Standby−Power Offline SMPS
IC4, IC5
IC6
L1, L2
Value
Manufacturer Part Number
T3,15A
T3,15A
NCP1653DR2
NCP1653DR2
NCP1395A
NCP1395A
NCP1012AP065
NCP1012AP065
PC817P
PC817P
TL431BILP
TL431BILP
2m7
PMEC103/V 2m7
Optocoupler
Adjustable Shunt Regulator 2.5−36 V/
1.0−100 mA
Common Mode Inductor
L3
Inductor
650uH
IND−PFC−260W−v1
L4
Inductor
1m5
RFB0810−152L
L5
Inductor
100uH
IND−LLC−v1
L6
Inductor
2.2uH
IND−FLT−2u2−10A
M1
N−Channel 600 V 0.140 W−20 A TO−220
SPA20N60C3
SPA20N60C3
M2, M3
N−Channel 550 V @ Tjmax−0.30 W − 12 A
TO−220FP
STP12NM50FP
STP12NM50FP
Q1
General Purpose Transistors NPN Silicon
BC846BLT1
BC846BLT1
R1
Axial Lead Resistor 3.0 W
0.1R
3W
R2, R7, R15,
R16
SMD Resistor
470k
CRCW1206
R3, R4
SMD Resistor
750k
CRCW1206
R5, R6
SMD Resistor
2M2
CRCW1206
R8, R22, R42
SMD Resistor
3k3
CRCW1206
R9
SMD Resistor
11k
CRCW1206
R10
SMD Resistor
4R7
CRCW1206
R12
SMD Resistor
56k
CRCW1206
R13, R40, R44
SMD Resistor
1k
CRCW1206
R14
SMD Resistor
300k
CRCW1206
R17
NU
R18
SMD Resistor
100k
CRCW1206
R19
SMD Resistor
680k
CRCW1206
R20
SMD Resistor
330k
CRCW1206
R21
SMD Resistor
150k
CRCW1206
R23,
STRAP 1, 2
SMD Resistor
0R
CRCW1206
R24
SMD Resistor
1M2
CRCW1206
R25
SMD Resistor
220k
CRCW1206
R26
SMD Resistor
33k
CRCW1206
R27
SMD Resistor
5k6
CRCW1206
R28
SMD Resistor
100R
CRCW1206
R29
NU
R30
SMD Resistor
56k
CRCW1206
R11, R31, R32
SMD Resistor
10k
CRCW1206
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NCP1395 Demo Board Parts List
Designator
R33
Description
SMD Resistor
R34
Value
Manufacturer Part Number
2k2
CRCW1206
NU
CRCW1206
R35
SMD Resistor
180R
CRCW1206
R36
SMD Resistor
1k2
CRCW1206
R37
NU
R38
NU
R39
NU
R41, R47
SMD Resistor
2k7
CRCW1206
R43
SMD Resistor
5k6
CRCW1206
R45
NU
R46
SMD Resistor
18k
CRCW1206
R48
High Ohmic, High Voltage Resistor
4M7
0.5W VR37 Series
RTH1
VDR1
NU
Voltage Dependent Resistor
CV 275 K 10
B1
CV 275 K 10 B 1
TR1
Transformer
TRAFO ETD29
TR−LLC−v3−24V
TR2
CS Transformer
CST1−100LB − CS
TR.
CST1−100LB − CS Tr.
H1
PCB Connector
NA
SVPS CEE7.5/3 Grey
H2
PCB Connector
NA
SVPS MV 252/5.08 Green
HS1
Heat Sink
NA
CHL01−BLK
HS2
Heat Sink
NA
SK 505 30 SA
Driver Module with NCP5181
R1
SMD Resistor
18R
CRCW1206
R2, R3
SMD Resistor
10R
CRCW1206
R4, R5
SMD Resistor
C1, C2
SMD Capacitor
0R
CRCW1206
100n
VJ1206Y104KXBAx
D1
Surface Mount Ultrafast Power Rectifier
MURA160
MURA160
IC1
Integrated Half Bridge Driver
NCP5181
NCP5181
Driver Module with Transformer
R1, R2
SMD Resistor
150R
CRCW1206
R3, R4
SMD Resistor
10k
CRCW1206
R5, R6
SMD Resistor
22R
CRCW1206
R7, R8
SMD Resistor
8R2
CRCW1206
STRAP
SMD Resistor
0R
CRCW1206
C1, C2
SMD Capacitor
100n
VJ1206Y104KXBAx
D1, D2, D3, D4
0.5 A 40 V Schottky Rectifier
D5, D6, D9,
D10
Small Signal Switch Diode 100 V
D7, D8, D11,
D12
Zener Diode 500 mW 18 V
MBR0540T1
MBR0540T1
MMSD4148T1
MMSD4148T1
MMSZ18T1
MMSZ18T1
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NCP1395 Demo Board Parts List
Driver Module with Transformer
Q1, Q3
General Purpose Transistors NPN Silicon
BC817−40LT1
BC817−40LT1
Q2, Q4, Q5, Q6
General Purpose Transistors PNP Silicon
BC807−40LT1
BC807−40LT1
NA
TR−DRW−01
TR1
Transformer
Please see the NCP1395A/B product folder on www.onsemi.com for PCB Gerber files and other collateral information regarding this demo
board.
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
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