NCP1256
www.onsemi.com
13
level does not properly collapse in presence of an
output short). In this controller, every time the internal
0.8−V maximum peak current limit is activated (or less
when OPP is used), an error flag is asserted and a time
period starts, thanks to the programmable timer. When
the timer has elapsed, the controller enters a
double−hiccup auto−recovery mode or is fully latched
depending on the selected option.
Please note that with the latched OCP option, the part
becomes sensitive to the UVLO event only at the first
power−on sequence. Any UVLO event is ignored
afterwards (normal auto−recovery operation). This is to pass
the pre−short test at power up:
1. if the internal error flag is armed (short circuit)
AND a UVLO event is sensed, the part is
immediately latched. UVLO sensing is ignored
after the first sucessful start−up sequence.
2. if an UVLO signal is detected but the error flag is
not asserted, double−hiccup auto−recovery occurs
and the part tries to resume operations.
3. if the error flag is asserted without UVLO, the part
classically permanently latches off.
Start−up Sequence
The NCP1256 start−up voltage is purposely made high to
permit large energy storage in a small V
cc
capacitor value.
This helps operate with a small start−up current which,
together with a small V
cc
capacitor, will not hamper the
start−up time. To further reduce the standby power, the
controller start−up current is purposely kept low, below
10 mA. Start−up resistors can therefore be connected to the
bulk capacitor or directly to the mains input voltage if you
wish to save a few more mW.
D1 D2
D3 D4
Input
mains
Cbulk
C1
X2
R1 R2
R3 R4
ICC1
CVcc
D5
1N4148
C4
D6
BAV21
aux
.
Vcc
I1
I2
I3
Figure 34. The startup resistor can be connected to the
input mains for further power dissipation reduction
Figure 34 shows a typical recommended configuration
where start−up resistors connect together to the mains input.
This technique offers the benefit of freely discharging the
X2 capacitor usually part of the EMI filter. The calculation
of these resistors depends on several parameters. Assuming
a 0.47−mF X2 capacitor, the safety standard recommends a
time constant less than 1 s maximum when a resistor is
connected in parallel to provide a discharge path. This sets
the upper limit for the sum of discharge resistors connected
to the controller V
cc
:
R
startup
t
1
0.47 m
t 2.1 MW
(eq. 1)
The first step starts with the calculation of the needed V
cc
capacitor which will supply the controller until the auxiliary
winding takes over. Experience shows that this time t
1
can
be between 5 and 20 ms. Considering that we need at least
an energy reservoir for a t
1
time of 10 ms, the V
cc
capacitor
must be larger than:
CV
CC
w
I
CC
t
1
VCC
on
* VCC
min
w
1.5 m 10 m
9
w 1.6 mF
(eq. 2)
Let us select a 2.2−mF capacitor at first and experiments
in the laboratory will let us know if we were too optimistic
for t
1
. Experiments across temperature range are important
as capacitance and ESR of this V
cc
capacitor can be affected.
The V
cc
capacitor being known, we can now evaluate the
charging current we need to bring the V
cc
voltage from 0 to
the IC VCC
on
voltage, 18 V typical. This current has to be
selected to ensure start−up at the lowest mains (85 V rms) to
be less than 3 s (2.5 s for design margin):
I
charge
w
VCC
on
C
V
CC
2.5
w
18 2.2 m
2.5
w 16 mA
(eq. 3)
If we account for the 10−mA current that will flow inside
the controller (I
1
in Figure 34), then the total charging
current delivered by the start−up resistor must be 26 mA,
rounded to 30 mA. If we connect the start−up network to both
NCP1256
www.onsemi.com
14
mains inputs (two half−wave connections then), half of the
average current I
1
is defined by:
I
1
2
+
V
ac,rms
2
Ǹ
p
* VCC
on
R
startup
(eq. 4)
To make sure this current is always greater than 15 mA
(half of the necessary 30−mA current), the minimum value
for R
start−up
can be extracted:
R
start−up
v
V
ac,rms
2
Ǹ
p
−VCC
on
I
CV
cc
,min
v
85 1.414
p
−18
15 m
v 1.3MW
(eq. 5)
We could thus connect two resistors of 1.3 MW (total 2.6
MW) across the line to a) power the IC at start up b) ensure
X2 discharge when the user unplugs the adapter.
This calculation is purely theoretical, considering a
constant charging current. In reality, the take over time at
start up can be shorter (or longer!) and it can lead to a
reduction of the V
cc
capacitor. This brings a decrease in the
charging current and an increase of the start−up resistor, for
the benefit of standby power. Laboratory experiments on the
prototype are thus mandatory to fine tune the converter. If we
chose the two 1−MW resistors as suggested by Equation 5,
the dissipated power per resistance at high line amounts to:
P
R
startup,max
[
V
ac,peak
2
4R
start−up
+
ǒ
230 2
Ǹ
Ǔ
2
4 1Meg
+
105k
4Meg
+ 26mW
(eq. 6)
or a total of 52 mW.
Now that the first V
cc
capacitor has been selected, we must
ensure that the self−supply does not disappear in no−load
conditions. In this mode, the skip−cycle can be so deep that
refreshing pulses are likely to be widely spaced, inducing a
large ripple on the V
cc
capacitor. If this ripple is too large,
chances exist to touch the VCC
(min)
and reset the controller
into a new start−up sequence. A solution is to grow this
capacitor but it will obviously be detrimental to the start−up
time. The option offered in Figure 34 elegantly solves this
potential issue by adding an extra capacitor on the auxiliary
winding. However, this component is separated from the V
cc
pin via a simple diode. You therefore have the ability to grow
this capacitor as you need to ensure the self−supply of the
controller without affecting the start−up time and standby
power.
Brown−Out Protection
Brown−out (BO) is a means to protect the converter
against an erratic behavior that can occur at the lowest input
voltage level. By safely stopping the output pulses when the
mains is below a predetermined value, the converter
prevents thermal runaway, greatly improving its robustness.
Brown−out protection is another way to avoid an erratic
hiccup mode when too low an input voltage limits the power
delivery. Some applications, such as printer power supplies,
forbid this kind of operations and impose a clean stop. In that
case, brown−out detection/protection is the way to go.
Figure 35 shows a simplified version of what is
implemented in the controller.
R1
1.4Meg
R2
80k
R3
1Meg
R4
1Meg
C1
1uF
L
N
To diode bridge
VBO
VccON
sync.
BO
Gnd
hysteresis
BO ok
Figure 35. A simple comparator monitors the input voltage via a single pin. When this voltage is too low, the
pulses are stopped and the V
cc
hiccups
NCP1256
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15
To ensure a clean re−start, the BO information is only
validated when V
cc
reaches VCC
ON
. This ensures a
fully−charged V
cc
capacitor when the controller pulses
again (fresh start up). An asynchronous BO−related re−start
could induce aborted start−up sequences if the V
cc
capacitor
would be too close to the UVLO threshold.
From the above schematic, the calculation of the resistor
is straightforward. We have connected the resistor to the
input line and thus observe a single−wave signal peaking to
V
in,peak
. The average voltage seen on top of R
4
in Figure 35
is:
V
in,avg
+
V
in,peak
p
(eq. 7)
Then, choose a bridge current compatible with the power
consumption you can accept. If we chose 10 mA, the
pull−down resistor R
2
calculation is straightforward:
R
2
+
V
BOon
I
bridge
+
0.8
10 m
+ 80 kW
(eq. 8)
Now suppose we want a typical turn−on voltage V
turn−on
of 80 V rms. From the two above equations, we can calculate
the value of the upper resistive string:
R
upper
+
ǒ
V
turn−on
2
Ǹ
p
Ǔ
−V
BOon
I
bridge
+
80 1.414
3.14
−0.8
10 m
+3.5MW
(eq. 9
)
The hysteresis on the internal reference source is 140 mV
typically. The ratio of the two voltages is 1.14. With the
upper resistive network, the turn−off voltage can then easily
be derived:
V
turn−off
+
V
turn−on
1.14
+
80
1.14
[ 70 V
(eq. 10)
A 1mF capacitor is necessary to filter out the input ripple.
Reducing its value, hence allowing more ripple, can help
fine−tune the hysteresis, if necessary. A simulation has been
run with an upper−side resistor of 3.7 MW, a lower−side
resistor of 80 kW and a 1−mF filtering capacitor. The
measured turn−on voltage is 80 V rms and the turn−off
voltage is around 70 V rms.
Please check the demonstration board schematic in which
the BO sensing is done in a slightly different way,
capitalizing on the X2 discharge resistors. Be aware that BO
test has to be carried without oscilloscope probes or any
leakage path that could affect the high−impedance sensing.
When the controller senses a BO event, all pulses are
immediately cut. The IC internal consumption brings V
cc
down towards UVLO. When this level is reached, the
controller goes back into low−consumption mode and lifts
V
cc
up again. At VCC
ON
, a check on the BO comparator is
made: if the input level is correct, the part re−starts, if still
too low, the part consumption brings V
cc
down again. As a
result, V
cc
operates in hiccup mode during a BO event.
The below figure describes the typical waveforms
obtained at start−up and in operation. Please note the
synchronization of the BO validation with the VCC
ON
point.
This ensures a clean start−up sequence with a fully charged
V
cc
capacitor.
V
cc
BO
DRV
BO is synced
to VCC
ON
.
A small delay
ensures BG is
ready.
Ok
Not Ok
Ok
Not Ok
t
t
t
VCC
ON
VCC
(min)
BO not Ok
V
cc
is
discharged
BO not Ok
V
cc
is
discharged
BO validated
BO is synced
to VCC
ON
.
Figure 36. the brown−out recovery is always synchronized to the V
cc
signal: when it reaches VCC
ON
, the driver delivers the output pulses.

NCP1256BSN65T1G

Mfr. #:
Manufacturer:
ON Semiconductor
Description:
Switching Controllers NCP1256B 65KHZ
Lifecycle:
New from this manufacturer.
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