LTC3634
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Figure 3. Setting the Output Voltage
APPLICATIONS INFORMATION
When RT is tied to INTV
CC
, the switching frequency will
default to approximately 2MHz, as set by an internal resis-
tor. This internal resistor is more sensitive to process and
temperature variations than an external resistor (see the
Typical Performance Characteristics section) and is best
used for applications where switching frequency accuracy
is not critical.
Output Voltage Programming
Each regulators output voltage is set by an external resis-
tive divider according to the following equation:
V
OUT
= V
FBREG
1+
R2
R1
where V
FBREG
is the reference voltage as specified in the
Electrical Characteristics Table. The reference voltage is
600mV for channel 1; for channel 2 the reference voltage
is equal to the VTTR pin voltage. The desired output volt-
age is set by appropriate selection of resistors R1 and R2
as shown in Figure 3.
The buffered output voltage on the VTTR pin is nominally
equal to half of the VDDQIN voltage; thus configuring V
OUT2
as a V
TT
bus termination supply for DDR memory is as
simple as shorting V
OUT2
to V
FB2
and connecting VDDQIN
directly to the V
OUT1
(the V
DDQ
supply).
Choosing large values for R1 and R2 will result in im-
proved zero-load efficiency but may lead to undesirable
noise coupling or phase margin reduction due to stray
capacitances at the V
FB
node. Care should be taken to
route the V
FB
trace away from any noise source, such as
the SW trace.
The LTC3634 controlled on-time architecture is optimized
for an output voltage range of 0.6V to 3V, which is suit-
able for powering DDR memory. The LTC3634 is capable
of regulating higher output voltages; however, controlled
on-time behavior is not ensured. When the output voltage
is greater than 3V, the step-down regulator is forced to
increase the switching frequency in order to achieve output
regulation. Furthermore, external clock synchronization is
no longer possible, and channel 2 cannot maintain 90°/180°
phase operation with respect to channel 1. In short, the
LTC3634 will behave like a constant on-time regulator
instead of a controlled on-time regulator. Therefore, output
voltages greater than 3V should only be used in applica-
tions where switching frequency and channel-to-channel
phase-locking are not critical performance characteristics.
Inductor Selection
For a given input and output voltage, the inductor value and
operating frequency determine the inductor ripple current.
More specifically, the inductor ripple current decreases
with higher inductor value or higher operating frequency
according to the following equation:
I
L
=
V
OUT
f L
1
V
OUT
V
IN
where ΔI
L
= inductor ripple current, f = operating frequency
and L = inductor value. A trade-off between component
size, efficiency and operating frequency can be seen from
this equation. Accepting larger values of ΔI
L
allows the
use of lower value inductors but results in greater inductor
LTC3634
R2
C
F
(OPTIONAL)
V
OUT
3634 F03
V
FB
SGND
R1
Figure 2. Switching Frequency vs R
T
0
FREQUENCY (kHz)
1000
2000
3000
5000
200
700600
3634 F02
0
6000
4000
100 300 400 500
R
T
RESISTOR (kΩ)
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APPLICATIONS INFORMATION
core loss, greater ESR loss in the output capacitor, and
larger output voltage ripple. Generally, highest efficiency
operation is obtained at low operating frequency with
small ripple current.
A reasonable starting point is to choose a ripple current
somewhere between 600mA and 1.2A peak-to-peak. Note
that the largest ripple current occurs at the highest V
IN
.
Exceeding 1.8A is not recommended in order to minimize
output voltage ripple. To guarantee that ripple current does
not exceed a specified maximum, the inductance should
be chosen according to:
L =
V
OUT
f I
L(MAX)
1
V
OUT
V
IN(MAX)
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 increases, core
losses decrease. Unfortunately, increased inductance
requires more turns of wire, leading to increased DCR
and copper loss.
Ferrite designs exhibit very low core loss and are pre-
ferred at high switching frequencies, so design goals
can concentrate on copper loss and preventing satura-
tion. 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, so it is important to ensure that
the core will not 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 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 versus size requirements
and any radiated field/EMI requirements. Table 1 gives a
sampling of available surface mount inductors.
Table 1. Inductor Selection Table
INDUCTANCE
(µH)
DCR
(mΩ)
MAX
CURRENT (A)
DIMENSIONS
(mm)
HEIGHT
(mm)
Würth Electronik WE-HC 744310 Series
0.24
0.55
0.95
1.15
2.00
2.1
3.8
6.4
9.0
14.0
18.0
14.0
11.0
8.5
6.5
7 × 7 3.3
Vishay IHLP-2020BZ-01 Series
0.22
0.33
0.47
0.68
1
5.2
8.2
8.8
12.4
20
15
12
11.5
10
7
5.2 × 5.5 2
Toko FDV0620 Series
0.20
0.47
1.0
4.5
8.3
18.3
12.4
9.0
5.7
7 × 7.7 2.0
Coilcraft D01813H Series
0.33
0.56
1.2
4
10
17
10
7.7
5.3
6 × 8.9 5.0
TDK RLF7030 Series
1.0
1.5
8.8
9.6
6.4
6.1
6.9 × 7.3 3.2
C
IN
and C
OUT
Selection
The input capacitance, C
IN
, is needed to filter the trapezoi-
dal wave current at the drain of the top power MOSFET.
To prevent large voltage transients from occurring, a low
ESR input capacitor sized for the maximum RMS current
is recommended. The maximum RMS current for a single
regulator is given by:
I
RMS
= I
OUT(MAX)
V
OUT
V
IN
V
OUT
( )
V
IN
When both regulators are active, the input current wave-
form is significantly different. Furthermore, the input RMS
current varies depending on each outputs load current as
well as whether V
TT
is sinking or sourcing current.
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When SW1 and SW2 operate 180° out-of-phase, the worst-
case input RMS current occurs when the V
TT
supply is
sinking current and V
DDQ
is sourcing the same amount of
current. Knowing that V
OUT2
= one-half V
OUT1
in the DDR
application, the input RMS current in this case is given by:
I
RMS
= I
OUT(MAX)
D1 1.5
D1
4
for D1 < 0.5
I
RMS
= I
OUT(MAX)
1
3
4
D1 for D1 > 0.5
where D1 is the duty cycle of channel 1 (V
DDQ
supply).
These equations show that maximum I
RMS
occurs at
50% duty cycle (V
IN
= 2 V
OUT1
). This simple worst-case
condition may be used for design as deviations in duty
cycle do not offer significant 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. For low input voltage
applications, sufficient bulk input capacitance is needed
to minimize transient effects during output load changes.
Even though the LTC3634 design includes an overvoltage
protection circuit, care must always be taken to ensure
input voltage transients do not pose an overvoltage haz-
ard to the part.
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. The output ripple, ΔV
OUT
, is
approximated by:
V
OUT
< I
L
ESR+
1
8 f C
OUT
When using low-ESR ceramic capacitors, it is more use-
ful to choose the output capacitor value to fulfill a charge
storage requirement. During a load step, the output capacitor
APPLICATIONS INFORMATION
must instantaneously supply the current to support the load
until the feedback loop raises the switch current enough
to support the load. The time required for the feedback
loop to respond is dependent on the compensation and
the output capacitor size. Typically, three to four cycles
are required to respond to a load step, but only in the first
cycle does the output drop linearly. The output droop,
V
DROOP
, is usually about three times the linear drop of
the first cycle, provided the loop crossover frequency is
maximized. Thus, a good place to start is with the output
capacitor size of approximately:
C
OUT
3 I
OUT
f V
DROOP
Though this equation provides a good approximation, more
capacitance may be required depending on the duty cycle
and load step requirements. The actual V
DROOP
should be
verified by applying a load step to the output.
Using Ceramic Input and Output Capacitors
Higher values, lower cost ceramic capacitors are available
in small case sizes. Their high ripple current, high voltage
rating and low ESR make them ideal for switching regulator
applications. However, due to the self-resonant and high-
Q characteristics of some types of ceramic capacitors,
care must be taken when these capacitors are used at
the input. 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
V
IN
input. 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. For
a more detailed discussion, refer to Application Note 88.
When choosing the input and output ceramic capacitors,
choose the X5R and X7R dielectric formulations. These
dielectrics have the best temperature and voltage char-
acteristics of all the ceramics for a given value and size.

LTC3634IFE#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 15V Dual 3A Monolithic Step Down Regulator for DDR Power
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