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IW1707 датащи(PDF) 8 Page - Dialog Semiconductor

номер детали IW1707
подробное описание детали  Low-Power Off-Line Digital Green-Mode PWM Controller
PDF  13 Pages
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iW1707
Low-Power Off-Line Digital Green-Mode PWM Controller
Rev. 0.2
iW1707
Page 8
MaRch 8, 2012
depletion NFET or BJT turns on, and the V
CC capacitor
begins to charge up again towards the start-up threshold to
initiate a new soft-start process.
In applications where the active start-up is not needed,
the start-up resistor can be directly connected to the V
CC
pin without using the active start-up device, and the ASU
pin can be left unconnected. Refer to Figure 3.3 for the
application circuit.
9.3 Understanding Primary Feedback
Figure 9.2 illustrates a simplified flyback converter. When
the switch Q1 conducts during t
ON(t), the current ig(t) is
directly drawn from rectified sinusoid v
g(t). The energy Eg(t)
is stored in the magnetizing inductance L
M. The rectifying
diode D1 is reverse biased and the load current I
O is
supplied by the secondary capacitor C
O. When Q1 turns off,
D1 conducts and the stored energy E
g(t) is delivered to the
output.
+
vin(t)
TS(t)
IO
VO
D1
Q1
N:1
VAUX
CO
vg(t)
ig(t)
+
iin(t)
id(t)
Figure 9.2: Simplified Flyback Converter
In order to tightly regulate the output voltage, the
information about the output voltage and load current need
to be accurately sensed. In the DCM flyback converter,
this information can be read via the auxiliary winding or
the primary magnetizing inductance (L
M).
During the Q1
on-time, the load current is supplied from the output filter
capacitor C
O. The voltage across LM is vg(t), assuming the
voltage dropped across Q1 is zero. The current in Q1 ramps
up linearly at a rate of:
( )
( )
gg
M
di t
v t
dt
L
=
(9.1)
At the end of on-time, the current has ramped up to:
( )
( )
_
g
ON
g peak
M
vt t
it
L
×
=
(9.2)
This current represents a stored energy of:
( )2
_
2
M
g
g peak
L
E
it
=
×
(9.3)
When Q1, turns off at t
O, ig(t) in LM forces a reversal of
polarities on all windings. Ignoring the communication-time
caused by the leakage inductance L
K at the instant of
turn-off t
O, the primary current transfers to the secondary at
a peak amplitude of:
( )
( )
_
P
d
g peak
S
N
i t
i
t
N
=
×
(9.4)
Assuming the secondary winding is master, and the auxiliary
winding is slave,
VAUX
0V
VAUX = -VIN x
NAUX
NP
VAUX = VO x
NAUX
NS
1
2
Figure 9.3: Auxiliary Voltage Waveforms
The auxiliary voltage is given by:
(
)
V
AUX
AUX
O
S
N
VV
N
=
+∆
(9.5)
and reflects the output voltage as shown in Figure 9.3.
The voltage at the load differs from the secondary voltage
by a diode drop and IR losses. Thus, if the secondary
voltage is always read at a constant secondary current, the
difference between the output voltage and the secondary
voltage will be a fixed ΔV. Furthermore, if the voltage can
be read when the secondary current is small, ΔV will also be
small. With the iW1707, ΔV can be ignored.
The real-time waveform analyzer in the iW1707 reads this
information cycle-by-cycle. The part then generates a
feedback voltage V
FB. The VFB signal precisely represents



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