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LT8494 Datasheet(PDF) 13 Page - Linear Technology

Part # LT8494
Description  SEPIC/Boost DC/DC Converter with 2A, 70V Switch, and 7關A Quiescent Current
PDF  26 Pages
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Manufacturer  LINER [Linear Technology]
Direct Link  http://www.linear.com
Logo LINER - Linear Technology

LT8494 Datasheet(HTML) 13 Page - Linear Technology

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LT8494
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For more information www.linear.com/LT8494
APPLICATIONS INFORMATION
For the coupled inductor SEPIC:
IL(PEAK) =IOUT • 1+
VOUT
VIN • η


+ VIN •DC
2•L • f
IL(AVG) =IOUT • 1+
VOUT
VIN • η
Note: Inductor current can be higher during load tran-
sients. It can also be higher during short-circuit and
start-up if inadequate soft-start capacitance is used. Thus,
IL(PEAK) may be higher than the switch current limit of
2.95A, and the RMS inductor current is approximately
equal to IL(AVG). Choose an inductor having sufficient
saturation current and RMS current ratings.
Capacitor Selection
Low ESR (equivalent series resistance) capacitors should
be used at the output to minimize the output ripple volt-
age. Multilayer ceramic capacitors are an excellent choice,
as they have an extremely low ESR and are available in
very small packages. X5R or X7R dielectrics are preferred,
as these materials retain their capacitance over wider volt-
age and temperature ranges. Always use a capacitor with
a sufficient voltage rating. Many capacitors rated at 2.2µF
to 20µF, particularly 0805 or 0603 case sizes, have greatly
reduced capacitance at the desired output voltage. Solid
tantalum or OS-CON capacitors can be used, but they will
occupy more board area than a ceramic and will have a
higher ESR with greater output ripple.
Ceramic capacitors also make a good choice for the input
decoupling capacitor, which should be placed as closely as
possible to the VIN and BIAS pins of the LT8494. A 2.2µF
to 4.7µF input capacitor is sufficient for most applications.
Audible Noise
Ceramic capacitors are small, robust and have very low
ESR. However, due to their piezoelectric nature, ceramic
capacitors can sometimes create audible noise when
used with the LT8494. During Burst Mode operation, the
LT8494 regulator’s switching frequency depends on the
load current, and at very light loads the regulator can
excite the ceramic capacitor at audio frequencies, gen-
erating audible noise. Since LT8494 operates at a lower
current limit during Burst Mode operation, the noise is
typically very quiet. If this is unacceptable, use a high per-
formance tantalum or electrolytic capacitor at the output.
Diode Selection
The diode used in boost or SEPIC topologies conducts
current only during the switch off-time. During the switch
on-time, the diode has reverse voltage across it. The peak
reverse voltage is equal to VOUT in the boost topology
and equal to (VOUT + VIN) in the SEPIC topology. Use a
diode with a reverse voltage rating greater than the peak
reverse voltage.
An additional consideration is the reverse leakage cur-
rent. The leakage current appears to the output as load
current and affects the efficiency, most noticeably, under
light load conditions. In Burst Mode operation, after the
inductor current vanishes, the reverse voltage across the
boost diode is approximately equal to VOUT – VIN in the
boost topology and VOUT in the SEPIC topology. The per-
centage of time that the diode is reverse biased increases
as load current decreases.
Schottky diodes that have larger forward voltages often
have less leakage, so a trade-off exists between light
load and high load efficiency. Also the Schottky diodes
with larger reverse bias ratings may have less leakage at
a given output voltage, therefore, superior leakage per-
formance can be achieved at the expense of diode size.
Finally, keep in mind that the leakage current of a power
Schottky diode goes up exponentially with junction tem-
perature. Therefore, the Schottky diode must be selected
with care to avoid excessive increase in light load supply
current at high temperatures.
Soft-Start
The LT8494 contains a soft-start circuit to limit peak
switch currents during start-up. High start-up current is
inherent in switching regulators since the feedback loop
is saturated due to VOUT being far from its final value. The



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