LTC3890
applicaTions inForMaTion
The equivalent resistance R1|| R2 is scaled to the room
temperature inductance and maximum DCR:
Accepting larger values of ∆I allows the use of low
L
inductances, but results in higher output voltage ripple
and greater core losses. A reasonable starting point for
L
R1||R2 =
setting ripple current is ∆I = 0.3(I
). The maximum
MAX
L
DCR at 20°C • C1
(
)
∆I occurs at the maximum input voltage.
L
The inductor value also has secondary effects. The tran-
sition to Burst Mode operation begins when the average
inductor current required results in a peak current below
The sense resistor values are:
R1||R2
RD
R1•RD
1– RD
R1=
; R2 =
25% of the current limit determined by R
. Lower
SENSE
inductor values (higher ∆I ) will cause this to occur at
L
The maximum power loss in R1 is related to duty cycle,
and will occur in continuous mode at the maximum input
voltage:
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 decrease.
V
IN(MAX) – VOUT • V
(
)
OUT
PLOSS R1=
R1
Inductor Core Selection
Once the value for L is known, the type of inductor must
be selected. High efficiency converters generally cannot
affordthecorelossfoundinlowcostpowderedironcores,
forcingtheuseofmoreexpensiveferriteormolypermalloy
cores. Actual core loss is independent of core size for a
fixedinductorvalue,butitisverydependentoninductance
value selected. As inductance increases, core losses go
down. Unfortunately, increased inductance requires more
turns of wire and therefore copper losses will increase.
Ensure that R1 has a power rating higher than this value.
If high efficiency is necessary at light loads, consider this
power loss when deciding whether to use DCR sensing or
sense resistors. Light load power loss can be modestly
higher with a DCR network than with a sense resistor, due
totheextraswitchinglossesincurredthroughR1.However,
DCR sensing eliminates a sense resistor, reduces conduc-
tion losses and provides higher efficiency at heavy loads.
Peak efficiency is about the same with either method.
Ferrite designs have very low core loss and are preferred
for high switching frequencies, so design goals can con-
centrate on copper loss and preventing saturation. Ferrite
core material saturates hard, which means that induc-
tance collapses abruptly when the peak design current is
exceeded. This results in an abrupt increase in inductor
ripple current and consequent output voltage ripple. Do
not allow the core to saturate!
Inductor Value Calculation
The operating frequency and inductor selection are inter-
related in that higher operating frequencies allow the use
of smaller inductor and capacitor values. So why would
anyone ever choose to operate at lower frequencies with
larger components? The answer is efficiency. A higher
frequency generally results in lower efficiency because of
MOSFET switching and gate charge losses. In addition to
this basic trade-off, the effect of inductor value on ripple
currentandlowcurrentoperationmustalsobeconsidered.
Power MOSFET and Schottky Diode
(Optional) Selection
Two external power MOSFETs must be selected for each
controller in the LTC3890: one N-channel MOSFET for the
top (main) switch, and one N-channel MOSFET for the
bottom (synchronous) switch.
The inductor value has a direct effect on ripple current. The
inductor ripple current, ∆I , decreases with higher induc-
L
tance or higher frequency and increases with higher V :
IN
VOUT
1
∆IL =
V
1–
OUT
f L
( ) ( )
V
IN
3890fb
17
Linear Systems [ Linear Systems ]
