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LTC3405A_15 Datasheet, PDF (8/16 Pages) Linear Technology – 1.5MHz, 300mA Synchronous Step-Down Regulator in ThinSOT
LTC3405A
APPLICATIO S I FOR ATIO
The basic LTC3405A application circuit is shown in Fig-
ure 1. External component selection is driven by the load
requirement and begins with the selection of L followed by
CIN and COUT.
Inductor Selection
For most applications, the value of the inductor will fall in
the range of 2.2µH to 10µH. Its value is chosen based on
the desired ripple current. Large value inductors lower
ripple current and small value inductors result in higher
ripple currents. Higher VIN or VOUT also increases the ripple
current as shown in equation 1. A reasonable starting point
for setting ripple current is ∆IL = 120mA (40% of 300mA).
∆IL
=
1
(f)(L)
VOUT ⎛⎝⎜1−
VOUT
VIN
⎞
⎠⎟
(1)
The DC current rating of the inductor should be at least
equal to the maximum load current plus half the ripple
current to prevent core saturation. Thus, a 360mA rated
inductor should be enough for most applications (300mA
+ 60mA). For better efficiency, choose a low DC-resistance
inductor.
The inductor value also has an effect on Burst Mode
operation. The transition to low current operation begins
when the inductor current peaks fall to approximately
100mA. Lower inductor values (higher ∆IL) will cause this
to occur at lower load currents, which can cause a dip in
efficiency in the upper range of low current operation. In
Burst Mode operation, lower inductance values will cause
the burst frequency to increase.
Inductor Core Selection
Different core materials and shapes will change the size/
current and price/current relationship of an inductor. Tor-
oid or shielded pot cores in ferrite or permalloy materials
are small and don’t radiate much energy, but generally cost
more than powdered iron core inductors with similar
Table 1. Representative Surface Mount Inductors
MAX DC
MANUFACTURER PART NUMBER VALUE CURRENT DCR HEIGHT
Taiyo Yuden
LB2016T2R2M
LB2012T2R2M
LB2016T3R3M
2.2µH 315mA 0.13Ω 1.6mm
2.2µH 240mA 0.23Ω 1.25mm
3.3µH 280mA 0.2Ω 1.6mm
Panasonic
ELT5KT4R7M 4.7µH 950mA 0.2Ω 1.2mm
Murata
LQH3C4R7M34 4.7µH 450mA 0.2Ω 2mm
Taiyo Yuden
LB2016T4R7M 4.7µH 210mA 0.25Ω 1.6mm
Panasonic
ELT5KT6R8M 6.8µH 760mA 0.3Ω 1.2mm
Panasonic
ELT5KT100M
10µH 680mA 0.36Ω 1.2mm
Sumida
CMD4D116R8MC 6.8µH 620mA 0.23Ω 1.2mm
electrical characteristics. The choice of which style induc-
tor to use often depends more on the price vs size require-
ments and any radiated field/EMI requirements than on
what the LTC3405A requires to operate. Table 1 shows
some typical surface mount inductors that work well in
LTC3405A applications.
CIN and COUT Selection
In continuous mode, the source current of the top MOSFET
is a square wave of duty cycle VOUT/VIN. To prevent large
voltage transients, a low ESR input capacitor sized for the
maximum RMS current must be used. The maximum
RMS capacitor current is given by:
[ ( )] CIN required IRMS ≅ IOMAX
VOUT VIN − VOUT
VIN
1/ 2
This formula has a maximum at VIN = 2VOUT, where
IRMS = IOUT/2. This simple worst-case condition is com-
monly used for design because even significant deviations
do not offer much relief. Note that the capacitor
manufacturer’s ripple current ratings are often based on
2000 hours of life. This makes it advisable to further derate
the capacitor, or choose a capacitor rated at a higher
temperature than required. Always consult the manufac-
turer if there is any question.
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