LTC3605
12
3605fh
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ripple current and consequent output voltage ripple. Do
not allow the core to saturate!
Different core materials and shapes will change the size/
current and price/current relationship of an inductor. Toroid
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
characteristics. The choice of which style inductor to use
mainly depends on the price versus size requirements
and any radiated field/EMI requirements. New designs for
surface mount inductors are available from Toko, Vishay,
NEC/Tokin, Cooper, TDK and Wurth Elektronik. Refer to
Table 1 for more details.
Checking Transient Response
The OPTI-LOOP compensation allows the transient re
-
sponse to be optimized for a wide range of loads and
output capacitors. The availability of the ITH pin not
only allows optimization of the control loop behavior but
also provides a DC-coupled and AC-filtered closed-loop
response test point. The DC step, rise time and settling
at this test point truly reflects the closed-loop response.
Assuming a predominantly second order system, phase
margin and/or damping factor can be estimated using the
percentage of overshoot seen at this pin.
The ITH external components shown in the circuit on the
first page of this data sheet provides an adequate starting
point for most applications. The series R-C filter sets the
dominant pole zero loop compensation. The values can
be modified slightly (from 0.5 to 2 times their suggested
values) to optimize transient response once the final PC
layout is done and the particular output capacitor type
and value have been determined. The output capacitors
need to be selected because their various types and values
determine the loop feedback factor gain and phase. An
output current pulse of 20% to 100% of full load current
having a rise time of 1µs to 10µs will produce output volt
-
age and ITH pin waveforms that will give a sense of the
overall loop stability without breaking the feedback loop.
Switching regulators take several cycles to respond to a
step in load current. When a load step occurs, V
OUT
im-
mediately shifts by an amount equal to DI
LOAD
• ESR, where
operaTion
Lower ripple current reduces core losses in the inductor,
ESR losses in the output capacitors and output voltage
ripple. Highest efficiency operation is obtained at low
frequency with small ripple current. However, achieving
this requires a large inductor. There is a trade-off between
component size, efficiency and operating frequency.
A reasonable starting point is to choose a ripple current
that is about 2.5A. This is especially important at low V
OUT
operation where V
OUT
is 1.8V or below. Care must be
given to choose an inductance value that will generate a
big enough current ripple (1.5A to 2.5A) so that the chip’s
valley current comparator has enough signal-to-noise ratio
to force constant switching frequency. Meanwhile, also note
that the largest ripple current occurs at the highest V
IN
. To
guarantee that ripple current does not exceed a specified
maximum, the inductance should be chosen according to:
L =
V
OUT
f • DI
L(MAX)
• 1–
V
OUT
V
IN(MAX)
⎛
⎝
⎜
⎜
⎞
⎠
⎟
⎟
However, the inductor ripple current must not be so large
that its valley current level (–∆I
L
/2) can exceed the negative
current limit, which can be as low as –3.5A. If the negative
current limit is exceeded in forced continuous mode of op
-
eration, V
OUT
can get charged to above the regulation level
until the inductor current no longer exceeds the negative
current limit. In such instances, choose a larger inductor
value to reduce the inductor ripple current. The alternative
is to reduce the R
T
resistor value to increase the switching
frequency in order to reduce the inductor ripple current.
Once the value for L is known, the type of inductor must
be selected. Actual core loss is independent of core size
for a fixed inductor value, but is very dependent on the
inductance selected. As the inductance or frequency in
-
creases, core losses decrease. Unfortunately, increased
inductance requires more turns of wire and therefore
copper losses will increase.
Ferrite designs have very low core losses and are pre
-
ferred at high switching frequencies, so design goals can
concentrate on copper loss and preventing saturation.
Ferrite core material saturates
“hard”, which means that
inductance collapses abruptly when the peak design current
is exceeded. This results in an abrupt increase in inductor