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LTC3411_15 Datasheet, PDF (9/24 Pages) Linear Technology – 1.25A, 4MHz, Synchronous Step-Down DC/DC Converter
LTC3411
APPLICATIONS INFORMATION
A general LTC3411 application circuit is shown in Figure 5.
External component selection is driven by the load require-
ment, and begins with the selection of the inductor L1.
Once L1 is chosen, CIN and COUT can be selected.
Operating Frequency
Selection of the operating frequency is a tradeoff between
efficiency and component size. High frequency operation
allows the use of smaller inductor and capacitor values.
Operation at lower frequencies improves efficiency by
reducing internal gate charge losses but requires larger
inductance values and/or capacitance to maintain low
output ripple voltage.
The operating frequency, fO, of the LTC3411 is determined
by an external resistor that is connected between the RT
pin and ground. The value of the resistor sets the ramp
current that is used to charge and discharge an internal
timing capacitor within the oscillator and can be calculated
by using the following equation:
RT = 9.78 •1011(fO )−1.08(Ω)
or can be selected using Figure 2.
The maximum usable operating frequency is limited by
the minimum on-time and the duty cycle. This can be
calculated as:
fO(MAX) ≈ 6.67 • (VOUT / VIN(MAX)) (MHz)
The minimum frequency is limited by leakage and noise
coupling due to the large resistance of RT.
Inductor Selection
Although the inductor does not influence the operat-
ing frequency, the inductor value has a direct effect on
ripple current. The inductor ripple current ΔIL decreases
with higher inductance and increases with higher VIN or
VOUT :
ΔIL
=
VOUT
fO• L
•
⎛⎝⎜1−
VOUT
V IN
⎞
⎠⎟
Accepting larger values of ΔIL allows the use of low induc-
tances, but results in higher output voltage ripple, greater
core losses, and lower output current capability.
A reasonable starting point for setting ripple current is 40%
of maximum output current, or ΔIL = 0.4 • 1.25A = 500mA.
The largest ripple current ΔIL occurs at the maximum input
voltage. To guarantee that the ripple current stays below a
specified maximum, the inductor value should be chosen
according to the following equation:
L
=
VOUT
f O• ΔIL
⎛
• ⎝⎜1−
VOUT ⎞
VIN(MAX) ⎠⎟
The inductor value will also have an effect on Burst Mode
operation. The transition from low current operation
begins when the peak inductor current falls below a level
set by the burst clamp. Lower inductor values result in
4.5 TA = 25°C
4.0
3.5
3.0
2.5
2.0
1.5
1.0
0.5
0
0
500
1000
1500
RT (kΩ)
3411 F02
Figure 2. Frequency vs RT
3411fb
9