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LT3573 Datasheet(PDF) 9 Page - Linear Technology

Part # LT3573
Description  Isolated Flyback Converter without an Opto-Coupler
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Manufacturer  LINER [Linear Technology]
Direct Link  http://www.linear.com
Logo LINER - Linear Technology

LT3573 Datasheet(HTML) 9 Page - Linear Technology

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LT3573
9
3573fd
For more information www.linear.com/LT3573
APPLICATIONS INFORMATION
ERROR AMPLIFIER—DYNAMIC THEORY
Due to the sampling nature of the feedback loop, there
are several timing signals and other constraints that are
required for proper LT3573 operation.
Minimum Current Limit
The LT3573 obtains output voltage information from the
SW pin when the secondary winding conducts current.
The sampling circuitry needs a minimum amount of time
to sample the output voltage. To guarantee enough time,
a minimum inductance value must be maintained. The
primary-side magnetizing inductance must be chosen
above the following value:
LPRI ≥ VOUT
tMIN
IMIN
•NPS = VOUT •NPS
1.4µH
V


tMIN = minimum off-time, 350ns
IMIN = minimum current limit, 250mA
The minimum current limit is higher than that on the Elec-
trical Characteristics table due to the overshoot caused by
the comparator delay.
Leakage Inductance Blanking
When the output switch first turns off, the flyback pulse
appears.However,ittakesafinitetimeuntilthetransformer
primary-side voltage waveform approximately represents
the output voltage. This is partly due to the rise time on
the SW node, but more importantly due to the trans-
former leakage inductance. The latter causes a very fast
voltage spike on the primary-side of the transformer that
is not directly related to output voltage (some time is also
required for internal settling of the feedback amplifier
circuitry). The leakage inductance spike is largest when
the power switch current is highest.
In order to maintain immunity to these phenomena, a fixed
delay is introduced between the switch turn-off command
andthebeginningofthesampling.Theblankingisinternally
set to 150ns. In certain cases, the leakage inductance may
not be settled by the end of the blanking period, but will
not significantly affect output regulation.
Selecting RFB and RREF Resistor Values
The expression for VOUT, developed in the Operation sec-
tion, can be rearranged to yield the following expression
for RFB:
RFB =
RREF •NPS VOUT + VF
(
)a+VTC


VBG
where,
VOUT = Output voltage
VF = Switching diode forward voltage
a = Ratio of Q1, IC to IE, typically 0.986
NPS = Effective primary-to-secondary turns ratio
VTC = 0.55V
The equation assumes the temperature coefficients of
the diode and VTC are equal, which is a good first-order
approximation.
Strictly speaking, the above equation defines RFB not as an
absolute value, but as a ratio of RREF. So, the next ques-
tion is, “What is the proper value for RREF?” The answer
is that RREF should be approximately 6.04k. The LT3573
is trimmed and specified using this value of RREF. If the
impedance of RREF varies considerably from 6.04k, ad-
ditional errors will result. However, a variation in RREF of
several percent is acceptable. This yields a bit of freedom
in selecting standard 1% resistor values to yield nominal
RFB/RREF ratios.
Tables 1-4 are useful for selecting the resistor values for
RREF and RFB with no equations. The tables provide RFB,
RREF and RTC values for common output voltages and
common winding ratios.
Table 1. Common Resistor Values for 1:1 Transformers
VOUT (V)
NPS
RFB (kΩ)
RREF (kΩ)
RTC (kΩ)
3.3
1.00
18.7
6.04
19.1
5
1.00
27.4
6.04
28
12
1.00
64.9
6.04
66.5
15
1.00
80.6
6.04
80.6
20
1.00
107
6.04
105


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