LTC3607
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For more information www.linear.com/LTC3607
block DiagraM
CONTROL
LOGIC
+
+
+
LEVEL
SHIFT
HV
ICMP
PV
IN1
SW1
PGND1
PGOOD1
PV
IN2
SW2
PGND2
PGOOD2
3607 BD
MODE/SYNC
RCMP
HV
LEVEL
SHIFT
OSC
LDO
3.3V
0.65V
BANDGAP
REFERENCE
0.55V
0.6V
CLK
MODE 3.3V
3MΩ
PGOOD1
0.55V
RUN1
SGND
RUN2
V
FB1
I
TH
SV
IN
V
FB2
UVCOMP
EA
OVCOMP
0.6V
0.65V
REGULATOR 1
REGULATOR 2 (IDENTICAL TO REGULATOR 1)
LTC3607
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For more information www.linear.com/LTC3607
operaTion
The LTC3607 uses a constant-frequency, peak current
mode architecture. The operating frequency is set at
2.25MHz and can be synchronized to an external oscillator
between 1MHz and 4MHz. Both channels share the same
clock and run in-phase. To suit a variety of applications,
the selectable MODE/SYNC pin allows the user to trade-
off ripple for efficiency.
The output voltage is set by an external divider returned
to the V
FB
pins. An error amplifier compares the divided
output voltage with a reference voltage of 0.6V and ad-
justs the peak inductor current accordingly. Overvoltage
an
d unde
rvoltage comparators will pull the independent
PGOOD outputs low if the output voltage is not within
±8.5%. The PGOOD outputs will go high 64 clock cycles
after achieving regulation and will go low 64 cycles after
falling out of regulation.
Whether in Burst Mode or pulse-skipping operation, the
overvoltage protection circuit is still enabled when the rest
of the regulator is asleep. Hence, if V
OUT
rises above the
overvoltage threshold, the regulator is forced out of sleep.
Main Control Loop
During normal operation, the top power switch (P-channel
MOSFET) is turned on at the beginning of a clock cycle
when the V
FB
voltage is below the reference voltage. The
current into the inductor and the load increases until the
current limit is reached. The switch turns off and energy
stored in the inductor flows through the bottom switch
(N-channel MOSFET) into the load until the next clock cycle.
The pe
ak inductor current is controlled by the internally
compensated ITH voltage, which is the output of the error
amplifier. This amplifier compares the V
FB
pin to the 0.6V
internal reference. When the load current increases, the
V
FB
voltage decreases slightly below the reference. This
decrease causes the error amplifier to increase the ITH
voltage until the average inductor current matches the
new load current.
The main control loop is shut down by pulling the RUN
pin to ground.
Low Current Operation
Two discontinuous-conduction modes (DCMs) are avail
-
able to control the operation of the LTC3607 at low output
currents. Both modes, Burst Mode operation and pulse-
skipping, automatically switch from continuous operation
to the selected mode when the load current is low.
To optimize efficiency, Burst Mode operation can be se
-
lected by floating the MODE/SYNC pin or setting it to 1V
o
r gre
ater. When the load is relatively light, the LTC3607
automatically switches into Burst Mode operation in which
the PMOS switch operates intermittently based on load
demand with a fixed peak inductor current. By running
cycles periodically, the switching losses, which are domi
-
nated by the gate charge losses of the power MOSFETs,
are minimized. The main control loop is interrupted when
the output voltage reaches the desired regulated value.
A voltage comparator trips when the ITH voltage drops
below an internal clamp voltage, shutting off the switch
and reducing the power. The output capacitor and the
inductor supply the power to the load until ITH exceeds
an internal clamp voltage, turning on the switch and the
main control loop, which starts another cycle.
To optimize ripple, pulse-skipping mode can be selected
by grounding the MODE/SYNC pin. In the LTC3607, pulse-
skipping mode is implemented similarly to Burst Mode
operation with the ITH clamp set to a lower internal clamp
voltage. This results in lower ripple than in Burst Mode
operation with the trade-off being slightly lower efficiency.
Dropout Operation
When the input supply voltage decreases toward the output
voltage, the duty cycle increases to 100% which is the
dropout condition. In dropout, the PMOS switch is turned
on continuously with the output voltage being equal to the
input voltage minus the voltage drops across the internal
P-channel MOSFET and the inductor.
LTC3607
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For more information www.linear.com/LTC3607
applicaTions inForMaTion
An important design consideration is that the R
DS(ON)
of the P-channel switch increases with decreasing input
supply voltage (see Typical Performance Characteristics).
Therefore, the user should calculate the power dissipation
when the LTC3607 is used at 100% duty cycle with low
input voltage (see Thermal Considerations in the Applica
-
tions Information section).
Low/High Supply Operation
The LTC3607 incorporates an undervoltage lockout circuit
which shuts down the part when the input voltage drops
below about 3.7V to prevent unstable operation.
A general LTC3607 application circuit is shown in Figure 1.
External component selection is driven by the load require-
ment, and begins with the selection of the inductor L. Once
the in
ductor is chosen, C
IN
and C
OUT
can be selected.
Inductor Selection
The operating frequency directly effects both the inductor
value, and the ripple current. The inductor ripple current
ΔI
L
decreases with higher frequency and/or inductance
and increases with higher V
IN
:
I
L
=
V
OUT
f
O
L
1–
V
OUT
V
IN
Accepting larger values of ΔI
L
allows the use of low
inductances, but results in higher output voltage ripple,
greater core losses, and lower output current capability.
A reasonable starting point for setting ripple current is
ΔI
L
= 0.4 • I
O(MAX)
, where I
O(MAX)
is the maximum rated
output current. The largest ripple current ΔI
L
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 =
V
OUT
f
O
I
L
1–
V
OUT
V
IN(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
higher ripple current which causes this transition to occur
at lower load currents. This causes a dip in efciency 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
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 elec
-
trical characteristics. The choice of which style inductor to
use often depends more on the price vs size requirements
and any radiated field/EMI requirements than on what the
LTC3607 requires to operate. Table 1 shows the websites
of several surface mount inductor manufacturers.
Table 1. Inductor Manufacturer
Coilcraft http://www.coilcraft.com/powersel_lowl.html
Cooper Bussmann http://www.cooperindustries.com/content/public/
en/bussmann/electronics/products/coiltronics_
inductorandtransformermagnetics.html
Würth Electronic http://katalog.we-online.com/en/pbs/browse/
Power-Magnetics/Speicherdrosseln
Murata http://www.murata.com/products/inductor/index.
html
TDK http://www.tdk.co.jp/tefe02/coil.htm
Vishay http://www.vishay.com/inductors/power-
inductors/
Sumida http://www.sumida.com/en/products/
power_main.php

LTC3607EMSE#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 15V Dual 600mA Monolithic Synchronous Step-Down DC/DC Regulator
Lifecycle:
New from this manufacturer.
Delivery:
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