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The basic LTC3418 application circuit is shown on the
front page of this data sheet. External component selection
is determined by the maximum load current and begins
with the selection of the operating frequency and inductor
value followed by C
IN
and C
OUT
.
Operating Frequency
Selection of the operating frequency is a trade-off 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 of the LTC3418 is determined
by an external resistor that is connected between the R
T
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:
R
OS C
=
7.3 10
10
f
Ω
2.5kΩ
Although frequencies as high as 4MHz are possible, the
minimum on-time of the LTC3418 imposes a minimum
limit on the operating duty cycle. The minimum on-time
is typically 80ns. Therefore, the minimum duty cycle is
equal to:
100 80ns f(Hz)
Inductor Selection
For a given input and output voltage, the inductor value
and operating frequency determine the ripple current. The
ripple current I
L
increases with higher V
IN
or V
OUT
and
decreases with higher inductance:
ΔI
L
=
V
OUT
fL
1
V
OUT
V
IN
Having a lower ripple current reduces the core losses in
the inductor, the ESR losses in the output capacitors and
the output voltage ripple. Highest efficiency operation is
achieved at low frequency with small ripple current. This,
however, requires a large inductor.
A reasonable starting point for selecting the ripple current
is I
L
= 0.4(I
MAX
). The largest ripple current occurs at the
highest V
IN
. To guarantee that the ripple current stays
below a specified maximum, the inductor value should
be chosen according to the following equation:
L =
V
OUT
fΔI
L(MAX)
1
V
OUT
V
IN(MAX)
The inductor value will also have an effect on Burst Mode
operation. The transition from low current operation be-
gins when the peak inductor current falls below a level
set by the burst clamp. Lower inductor values result in
higher
ripple
current which causes this to occur at lower
load currents. This causes 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
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 it is very dependent on the
inductance selected. As the inductance increases, 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
ripple current and consequent output voltage ripple. Do
not allow the core to saturate!
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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 dont 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 vs size requirements and any
radiated field/EMI requirements. New designs for surface
mount inductors are available from Coiltronics, Coilcraft,
Toko and Sumida.
C
IN
and C
OUT
Selection
The input capacitance, C
IN
, is needed to filter the trapezoidal
wave current at the source of the top MOSFET. To prevent
large voltage transients from occurring, a low ESR input
capacitor sized for the maximum RMS current should be
used. The maximum RMS current is given by:
I
RMS
=I
OUT(MAX)
V
OUT
V
IN
V
IN
V
OUT
1
This formula has a maximum at V
IN
= 2V
OUT
, where I
RMS
=
I
OUT
/2. This simple worst-case condition is commonly used
for design because even significant deviations do not offer
much relief. Note that ripple current ratings from capacitor
manufacturers are often based on only 2000 hours of life
which makes it advisable to further derate the capacitor,
or choose a capacitor rated at a higher temperature than
required. Several capacitors may also be paralleled to meet
size or height requirements in the design.
The selection of C
OUT
is determined by the effective series
resistance (ESR) that is required to minimize voltage ripple
and load step transients as well as the amount of bulk
capacitance that is necessary to ensure that the control
loop is stable. Loop stability can be checked by viewing
the load transient response as described in a later section.
The output ripple, V
OUT
, is determined by:
ΔV
OUT
ΔI
L
ESR+
1
8fC
OUT
The output ripple is highest at maximum input voltage
since I
L
increases with input voltage. Multiple capacitors
placed in parallel may be needed to meet the ESR and
RMS current handling requirements. Dry tantalum, special
polymer, aluminum electrolytic and ceramic capacitors are
all available in surface mount packages. Special polymer
capacitors offer very low ESR but have lower capacitance
density than other types. Tantalum capacitors have the
highest capacitance density but it is important to only
use types that have been surge tested for use in switching
power supplies. Aluminum electrolytic capacitors have
significantly higher ESR, but can be used in cost-sensitive
applications provided that consideration is given to ripple
current ratings and long term reliability. Ceramic capaci
-
tors have excellent low ESR characteristics but can have
a high voltage coefficient and audible piezoelectric effects.
The high Q of ceramic capacitors with trace inductance
can also lead to significant ringing.
Using Ceramic Input and Output Capacitors
Higher values, lower cost ceramic capacitors are now
becoming available in smaller case sizes. Their high ripple
current, high voltage
rating and low ESR make them ideal
for switching regulator applications. However, care must
be taken when these capacitors are used at the input and
output. When a ceramic capacitor is used at the input and
the power is supplied by a wall adapter through long wires,
a load step at the output can induce ringing at the input,
V
IN
. At best, this ringing can couple to the output and be
mistaken as loop instability. At worst, a sudden inrush
of current through the long wires can potentially cause
a voltage spike at V
IN
large enough to damage the part.
When choosing the input and output ceramic capacitors,
choose the X5R or X7R dielectric formulations. These
dielectrics have the best temperature and voltage char
-
acteristics of all the ceramics for a given value and size.
Output Voltage Programming
The output voltage is set by an external resistive divider
according to the following equation:
V
OUT
= 0.8 1+
R2
R1
The resistive divider allows pin V
FB
to sense a fraction of
the output voltage as shown in Figure 1.
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Burst Clamp Programming
If the voltage on the SYNC/MODE pin is less than V
IN
by
1V, Burst Mode operation is enabled. During Burst Mode
operation, the voltage on the SYNC/MODE pin determines
the burst clamp level, which sets the minimum peak in
-
ductor current, I
BURST
, for each switching cycle. A graph
showing the relationship between the minimum peak
inductor current and the voltage on the SYNC/MODE pin
can be found in the Typical Performance Characteristics
section. In the graph, V
BURST
is the voltage on the SYNC/
MODE pin. I
BURST
can only be programmed in the range
of 0A to 10A. For values of V
BURST
less than 0.4V, I
BURST
is set at 0A. As the output load current drops, the peak
inductor currents decrease to keep the output voltage in
regulation. When the output load current demands a peak
inductor current that is less than I
BURST
, the burst clamp will
force the peak inductor current to remain equal to I
BURST
regardless of further reductions in the load current. Since
the average inductor current is greater than the output load
current, the voltage on the I
TH
pin will decrease. When
the I
TH
voltage drops to 350mV, sleep mode is enabled
in which both power MOSFETs are shut off and switching
action is discontinued to minimize power consumption.
All circuitry is turned back on and the power MOSFETs
begin switching again when the output voltage drops out
of regulation. The value for I
BURST
is determined by the
desired amount of output voltage ripple. As the value of
I
BURST
increases, the sleep period between pulses and the
output voltage ripple increase. The burst clamp voltage,
V
BURST
, can be set by a resistor divider from the V
FB
pin
to the SGND pin as shown in the Typical Application on
the front page of this data sheet.
Pulse skipping, which is a compromise between low output
voltage ripple and efficiency during low load current opera
-
tion, can be implemented by connecting the SYNC/MODE
V
FB
V
OUT
R1
3418 F01
R2
SGND
LTC3418
Figure 1. Setting the Output Voltage
pin to ground. This sets I
BURST
to 0A. In this condition, the
peak inductor current is limited by the minimum on-time
of the current comparator; and the lowest output voltage
ripple is achieved while still operating discontinuously.
During very light output loads, pulse skipping allows only
a few switching cycles to be skipped while maintaining
the output voltage in regulation.
Voltage Tracking
The LTC3418 allows the user to program how its output
voltage ramps during start-up by means of the TRACK
pin. Through this pin, the output voltage can be set up to
either track coincidentally or ratiometrically follow another
output voltage as shown in Figure 2. If the voltage on the
TRACK pin is less than 0.8V, voltage tracking is enabled.
During voltage tracking, the output voltage regulates to
the tracking voltage through a resistor divider network.
V
OUT2
V
OUT1
3418 F02a
TIME
OUTPUT VOLTAGE
V
OUT2
V
OUT1
3418 F02a
TIME
OUTPUT VOLTAGE
Figure 2a. Coincident Tracking
Figure 2b. Ratiometric Sequencing
applicaTions inForMaTion

LTC3418EUHF#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 8A, 4MHz, Mono Sync Buck Reg
Lifecycle:
New from this manufacturer.
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