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IW3602 датащи(PDF) 11 Page - Dialog Semiconductor

номер детали IW3602
подробное описание детали  AC/DC Digital Power Controller for Dimmable LED Drivers
PDF  19 Pages
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производитель  DIALOG [Dialog Semiconductor]
домашняя страница  http://www.dialog-semiconductor.com/
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IW3602 датащи(HTML) 11 Page - Dialog Semiconductor

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iW3602
AC/DC Digital Power Controller for
Dimmable LED Drivers
Rev. 1.0
iW3602
© 2015 Dialog Semiconductor (UK) Ltd.
Datasheet
11 of 19
VCC
VCC(ST)
ENABLE
Start-up
Sequencing
VIN
Figure 9.7 : Start-up Sequencing Diagram
9.6 Understanding Primary Feedback
Figure 9.8 illustrates a simplified flyback converter. When
the switch Q1 conducts during tON(t), the current ig(t) is
directly drawn from rectified vg(t). The energy Eg(t) is stored
in the magnetizing inductance LM. The rectifying diode D1 is
reversely biased and the load current IO is supplied by the
secondary capacitor CO. When Q1 turns off, D1 conducts and
the stored energy Eg(t) is delivered to the output.
+
vin(t)
TS(t)
IO
VO
VAUX
N:1
D1
Q1
VAUX
CO
vg(t)
ig(t)
+
–
iin(t)
id(t)
Figure 9.8 : Simplified Flyback Converter
In order to tightly regulate the output voltage, the information
about the output voltage and load current must be accurately
sensed. In the DCM flyback converter, this information can
be read via the auxiliary winding or the primary magnetizing
inductance (LM). During the Q1 on-time, the load current
is supplied from the output filter capacitor CO. 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:
()
()
g
g
M
di t
v t
dt
L
=
(9.6)
At the end of on-time, the current ramps up to:
_
()
()
g
ON
g peak
M
vt t
i
t
L
×
=
(9.7)
This current represents a stored energy of:
2
_
()
2
M
g
g peak
L
E
i
t
=
×
(9.8)
When Q1 turns off, ig(t) in LM forces a reversal of polarities on
all windings. Ignoring the communication-time caused by the
leakage inductance LK at the instant of turn-off, the primary
current transfers to the secondary at a peak amplitude of:
_
()
()
P
d
g peak
S
N
i t
i
t
N
=
×
(9.9)
Assuming the secondary winding is master and the auxiliary
winding is slave.
VAUX
0V
VAUX = -VIN x
NAUX
NP
VAUX = VO x
NAUX
NS
Figure 9.9 : Auxiliary Voltage Waveforms
The auxiliary voltage is given by:
()
AUX
AUX
O
S
N
V
VV
N
=
+∆
(9.10)
and reflects the output voltage as shown in Figure 9.9.
The voltage at the load differs from the secondary voltage by
a diode drop and IR losses. The diode drop is a function of
current, as are 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 is a
fixed ΔV. If the voltage can be read when the secondary
current is small, for example, at the knee of the auxiliary
waveform (see Figure 9.9), then ΔV is also small. With the
iW3602, ΔV can be ignored.
The real-time waveform analyzer in the iW3602 reads the
auxiliary waveform information cycle by cycle. The part then
generates a feedback voltage VFB. The VFB signal precisely



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