LTC3407A
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OPERATION
The LTC3407A uses a constant frequency, current mode
architecture. The operating frequency is set at 1.5MHz
and can be synchronized to an external oscillator. 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 noise for effi ciency.
The output voltage is set by an external divider returned
to the V
FB
pins. An error amplifi er compares the divided
output voltage with a reference voltage of 0.6V and adjusts
the peak inductor current accordingly. Overvoltage and
undervoltage comparators will pull the POR output low if
the output voltage is not within ±8.5%. The POR output
will go high after 65,536 clock cycles (about 44ms in pulse
skipping mode) of achieving regulation.
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 fl ows through the bottom switch (N-channel
MOSFET) into the load until the next clock cycle.
The peak inductor current is controlled by the internally
compensated I
TH
voltage, which is the output of the er-
ror amplifi er.This amplifi er compares the V
FB
pin to the
0.6V reference. When the load current increases, the
V
FB
voltage decreases slightly below the reference. This
decrease causes the error amplifi er to increase the I
TH
voltage until the average inductor current matches the
new load current.
The main control loop is shut down by pulling the RUN/SS
pin to ground.
Low Current Operation
Two modes are available to control the operation of the
LTC3407A at low currents. Both modes automatically
switch from continuous operation to the selected mode
when the load current is low.
To optimize effi ciency, the Burst Mode operation can be
selected. When the load is relatively light, the LTC3407A
automatically switches into Burst Mode operation in which
the PMOS switch operates intermittently based on load
demand with a fi xed 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 I
TH
is below 0.65V, shutting
off the switch and reducing the power. The output capaci-
tor and the inductor supply the power to the load until I
TH
exceeds 0.65V, turning on the switch and the main control
loop which starts another cycle.
For lower ripple noise at low currents, the pulse skipping
mode can be used. In this mode, the LTC3407A continues
to switch at a constant frequency down to very low cur-
rents, where it will begin skipping pulses.
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.
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 LTC3407A is used at 100% duty cycle with low
input voltage (See Thermal Considerations in the Applica-
tions Information Section).
Low Supply Operation
The LTC3407A incorporates an undervoltage lockout circuit
which shuts down the part when the input voltage drops
below about 1.65V to prevent unstable operation.
A general LTC3407A application circuit is shown in
Figure 1. External component selection is driven by the
load requirement, and begins with the selection of the
inductor L. Once the inductor is chosen, C
IN
and C
OUT
can be selected.
LTC3407A
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Inductor Selection
Although the inductor does not infl uence the operat-
ing frequency, the inductor value has a direct effect on
ripple current. The inductor ripple current ΔI
L
decreases
with higher inductance and increases with higher V
IN
or
V
OUT
:
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
=
0.3 • I
LIM
, where I
LIM
is the peak switch current limit. The
largest ripple current ΔI
L
occurs at the maximum input
voltage. To guarantee that the ripple current stays below a
specifi ed 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 effi ciency 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 characterisitics. The choice of which style inductor
to use often depends more on the price vs size require-
ments and any radiated fi eld/EMI requirements than on
what the LTC3407A requires to operate. Table 1 shows
some typical surface mount inductors that work well in
LTC3407A applications.
Table 1. Representative Surface Mount Inductors
MANUF-
ACTURER PART NUMBER VALUE
MAX DC
CURRENT DCR HEIGHT
Taiyo
Yuden
CB2016T2R2M
CB2012T2R2M
CB2016T3R3M
2.2µH
2.2µH
3.3µH
510mA
530mA
410mA
0.13
0.33
0.27
1.6mm
1.25mm
1.6mm
Panasonic ELT5KT4R7M 4.7µH 950mA 0.2 1.2mm
Sumida CDRH2D18/LD 4.7µH 630mA 0.086 2mm
Murata LQH32CN4R7M23 4.7µH 450mA 0.2 2mm
Taiyo
Yuden
NR30102R2M
NR30104R7M
2.2µH
4.7µH
1100mA
750mA
0.1
0.19
1mm
1mm
FDK FDKMIPF2520D
FDKMIPF2520D
FDKMIPF2520D
4.7µH
3.3µH
2.2µH
1100mA
1200mA
1300mA
0.11
0.1
0.08
1mm
1mm
1mm
TDK VLF3010AT4R7-
MR70
VLF3010AT3R3-
MR87
VLF3010AT2R2-
M1R0
4.7µH
3.3µH
2.2µH
700mA
870mA
1000mA
0.28
0.17
0.12
1mm
1mm
1mm
Input Capacitor (C
IN
) Selection
In continuous mode, the input current of the converter is a
square wave with a duty cycle of approximately V
OUT
/V
IN
.
To prevent large voltage transients, a low equivalent series
resistance (ESR) input capacitor sized for the maximum
RMS current must be used. The maximum RMS capacitor
current is given by:
I
RMS
I
MAX
V
OUT
(V
IN
–V
OUT
)
V
IN
where the maximum average output current I
MAX
equals
the peak current minus half the peak-to-peak ripple cur-
rent, I
MAX
= I
LIM
ΔI
L
/2.
APPLICATIONS INFORMATION
Figure 1. LTC3407A General Schematic
V
OUT2
RUN/SS2
V
IN
V
IN
= 2.5V TO 5.5V
V
OUT1
RUN/SS1
POR
SW1
V
FB1
GND
V
FB2
SW2
MODE/SYNC
LTC3407A
C
IN
R7
POWER-ON
RESET
C1C2
L1
L2
R4 R2
R1
R3
C
OUT2
C4 C3
C
OUT1
3407A F01
PULSESKIP*
BURST*
*MODE/SYNC = 0V: PULSE SKIP
MODE/SYNC = V
IN
: Burst Mode
R6 R5
LTC3407A
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APPLICATIONS INFORMATION
This formula has a maximum at V
IN
= 2V
OUT
, where I
RMS
= I
OUT
/2. This simple worst-case is commonly used to
design because even signifi cant deviations do not offer
much relief. Note that capacitor manufacturers ripple cur-
rent ratings are often based on only 2000 hours lifetime.
This 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
the size or height requirements of the design. An additional
0.1µF to 1µF ceramic capacitor is also recommended on
V
IN
for high frequency decoupling, when not using an all
ceramic capacitor solution.
Output Capacitor (C
OUT
) Selection
The selection of C
OUT
is driven by the required ESR to
minimize voltage ripple and load step transients. Typically,
once the ESR requirement is satisfi ed, the capacitance
is adequate for fi ltering. The output ripple (ΔV
OUT
) is
determined by:
V
OUT
I
L
ESR +
1
8f
O
C
OUT
where f
O
= operating frequency, C
OUT
= output capacitance
and ΔI
L
= ripple current in the inductor. The output ripple
is highest at maximum input voltage since ΔI
L
increases
with input voltage. With ΔI
L
= 0.3 • I
LIM
the output ripple
will be less than 100mV at maximum V
IN
and f
O
= 1.5MHz
with:
ESR
COUT
< 150m
Once the ESR requirements for C
OUT
have been met, the
RMS current rating generally far exceeds the I
RIPPLE(P-P)
requirement, except for an all ceramic solution.
In surface mount applications, multiple capacitors may
have to be paralleled to meet the capacitance, ESR or
RMS current handling requirement of the application.
Aluminum electrolytic, special polymer, ceramic and dry
tantulum capacitors are all available in surface mount
packages. The OS-CON semiconductor dielectric capacitor
available from Sanyo has the lowest ESR(size) product
of any aluminum electrolytic at a somewhat higher price.
Special polymer capacitors, such as Sanyo POSCAP, of-
fer very low ESR, but have a lower capacitance density
than other types. Tantalum capacitors have the highest
capacitance density. However, they also have a larger
ESR and it is critical that they are surge tested for use in
switching power supplies. An excellent choice is the AVX
TPS series of surface mount tantalums, available in case
heights ranging from 2mm to 4mm. Aluminum electrolytic
capacitors have a signifi cantly larger ESR, and are often
used in extremely cost-sensitive applications provided that
consideration is given to ripple current ratings and long
term reliability. Ceramic capacitors have the lowest ESR
and cost, but also have the lowest capacitance density,
a high voltage and temperature coeffi cient, and exhibit
audible piezoelectric effects. In addition, the high Q of
ceramic capacitors along with trace inductance can lead
to signifi cant ringing. Other capacitor types include the
Panasonic Special Polymer (SP) capacitors.
In most cases, 0.1µF to 1µF of ceramic capacitors should
also be placed close to the LTC3407A in parallel with the
main capacitors for high frequency decoupling.
Ceramic Input and Output Capacitors
Higher value, lower cost ceramic capacitors are now be-
coming available in smaller case sizes. These are tempting
for switching regulator use because of their very low ESR.
Unfortunately, the ESR is so low that it can cause loop
stability problems. Solid tantalum capacitor ESR gener-
ates a loop “zero” at 5kHz to 50kHz that is instrumental in
giving acceptable loop phase margin. Ceramic capacitors
remain capacitive to beyond 300kHz and usually resonate
with their ESL before ESR becomes effective. Also, ceramic
caps are prone to temperature effects which requires the
designer to check loop stability over the operating tem-
perature range. To minimize their large temperature and
voltage coeffi cients, only X5R or X7R ceramic capacitors
should be used. A good selection of ceramic capacitors
is available from Taiyo Yuden, TDK, and Murata.
Great care must be taken when using only ceramic input
and output capacitors. When a ceramic capacitor is used
at the input and the power is being supplied through long
wires, such as from a wall adapter, a load step at the output
can induce ringing at the V
IN
pin. At best, this ringing can
couple to the output and be mistaken as loop instability.
At worst, the ringing at the input can be large enough to
damage the part.

LTC3407AEMSE#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Dual. Sync. 600mA, 1.5MHz Step-dwn Convrtr
Lifecycle:
New from this manufacturer.
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