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PQ-42614 Datasheet(PDF) 2 Page - Fairchild Semiconductor

Part # PQ-42614
Description  Design Guideline for Single-Stage Flyback AC-DC Converter Using FL6961 for LED Lighting
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Manufacturer  FAIRCHILD [Fairchild Semiconductor]
Direct Link  http://www.fairchildsemi.com
Logo FAIRCHILD - Fairchild Semiconductor

PQ-42614 Datasheet(HTML) 2 Page - Fairchild Semiconductor

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AN-9737
APPLICATION NOTE
© 2011 Fairchild Semiconductor Corporation
www.fairchildsemi.com
Rev. 1.0.0 • 4/13/11
2
Figure 2 shows typical waveforms of the simplified circuit
of a flyback converter with CRM. When the MOSFET (Q1)
turns on, the primary current in primary side linearly
increases and is clamped at a certain internal level because
the FL6961 doesn’t have cycle-by-cycle current limit like a
conventional current mode control IC (such as FAN7527B).
Its peak level is determined by the primary magnetizing
inductance value and the fixed on-time. Instead of the cycle-
by-cycle primary current limit, the FL6961 has an over-
current protection (OCP) function. If the current sensing
signal is larger than internal detection level, the FL6961
doesn’t get output signal for operating the MOSFET (Q1).
Figure 2. Key Waveforms of Flyback Converter on
CRM
The FL6961 has a constant on-time across the whole range.
The input average current always follows the peak input
current, as shown in the equation:
ON
PK
MOSFET
AVG
t
I
I
2
1
)
(
=
(1)
This is also proportional to the instantaneous input voltage.
This means the input current shape is always the same as the
input voltage shape. The reverse diode voltage is linearly
increased and is equal to:
P
S
IN
O
DIODE
PK
N
N
V
V
V
+
=
)
(
(2)
During the MOSFET off-time, which is also the diode on-
time; the input current instantly drops to zero, the diode in
the secondary side conducts, and the diode current linearly
decreases. The peak current of the secondary side is the
same as the multiplication of the primary peak current and
turns ratio between the primary side (NP) and secondary side
(NS) and naturally decreases to zero. The average current of
the secondary side is:
off
PK
S
P
DIODE
AVG
t
I
N
N
I
2
1
)
(
=
(3)
Since the diode forward-voltage drop decreases as current
decreases, the output voltage reflects the primary winding
and adds additional voltage due to overshoot made by
resonance between the leakage inductance on primary-side
winding and parasitic capacitance on the MOSFET (Q1). As
a result, a superimposed voltage occurs on the MOSFET
during off-time as:
OS
R
IN
off
MOSFET
V
V
V
V
+
+
=
)
(
(4)
where VR is the reflected voltage and VOS is the voltage
overshoot term.
The reflected voltage, VR, is affected by the turns ratio
between the primary and secondary side of the transformer
and the output voltage, calculated as:
O
S
P
R
V
N
N
V =
(5)
Figure 3 shows the ideal waveforms of the primary-side
current at MOSFET (Q1) and the secondary-side current at
the diode. The input peak and average current on the
primary
side
follows
input
voltage
instantaneously.
Normally, secondary-side current on the diode is larger than
the primary side because of the turns ratio.
Figure 3. Ideal Waveforms
time
time
time
IPK ( MOSFET )
IDS (MOSFET Drain-to-Source Current))
ID (Diode Current)
VDS (MOSFET Voltage)
tON
tOFF
tS
IAVG (MOSFET )
IPK ( DIODE )
IAVG (DIODE )
VIN
VR
VOS


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