The LT®1610 is a micropower fixed frequency DC/DC
converter that operates from an input voltage as low as 1V.
Intended for small, low power applications, it switches at
1.7MHz, allowing the use of tiny capacitors and inductors.
The device can generate 3V at 30mA from a single cell
(1V) supply. An internal compensation network can be
connected to the LT1610’s VC pin, eliminating two external components. No-load quiescent current of the LT1610
is 30µA, and the internal NPN power switch handles a
300mA current with a voltage drop of 300mV.
The LT1610 is available in 8-lead MSOP and SO packages.
Error Amp Transconductance∆I = 2µA25µmhos
Error Amp Voltage Gain100V/V
Switching Frequency●1.41.72MHz
Maximum Duty Cycle778095%
= 1.5V, Not Switching3060µA
SHDN
= 0V, VIN = 2V0.010.5µA
SHDN
= 0V, VIN = 5V0.011.0µA
V
SHDN
≤ 2V (70°C)2%/V
1V ≤ V
IN
2V ≤ V
≤ 8V (25°C, 0°C)0.030.15%/V
IN
≤ 8V (70°C)0.2%/V
2V ≤ V
IN
●7595%
2
LT1610
LECTRICAL CCHARA TERIST
E
range, otherwise specifications are at T
= 25°C. Commercial grade 0°C to 70°C, V
A
ICS
The ● denotes specifications which apply over the specified temperature
= 1.5V, V
IN
= VIN, unless otherwise noted.
SHDN
(Note 2)
PARAMETERCONDITIONSMINTYPMAXUNITS
Switch Current Limit(Note 3)450600900mA
Switch V
CESAT
Switch Leakage CurrentVSW = 5V0.011µA
SHDN Input Voltage High1V
SHDN Input Voltage Low0.3V
SHDN Pin Bias CurrentV
ISW = 300mA300350mV
●400mV
= 3V10µA
SHDN
= 0V0.010.1µA
V
SHDN
The ● denotes specifications which apply over the specified temperature range, otherwise specifications are at TA = 25°C.
Industrial grade –40°C to 85°C, V
PARAMETERCONDITIONSMINTYPMAXUNITS
Minimum Operating VoltageTA = 85°C0.91V
Maximum Operating Voltage8V
Feedback Voltage●1.201.231.26V
Quiescent Current3060µA
Quiescent Current in ShutdownV
Error Amp Transconductance∆I = 2µA25µmhos
Error Amp Voltage Gain100V/V
Switching Frequency(Note 4)●1.41.72MHz
Maximum Duty Cycle(Note 4)778095%
Switch Current Limit450600900mA
Switch V
CESAT
Switch Leakage CurrentVSW = 5V0.011µA
SHDN Input Voltage High1V
SHDN Input Voltage Low0.3V
SHDN Pin Bias CurrentV
= 1.5V, V
IN
= VIN, unless otherwise noted.
SHDN
= –40°C1.25V
T
A
= 0V, VIN = 2V0.010.5µA
SHDN
= 0V, VIN = 5V0.011.0µA
V
SHDN
≤ 8V (85°C)0.2%/V
2V ≤ V
IN
●7595%
ISW = 300mA300350mV
●400mV
= 3V10µA
SHDN
V
= 0V0.010.1µA
SHDN
Note 1: Absolute Maximum Ratings are those values beyond which the life
of a device may be impaired.
Note 2: The LT1610C is guaranteed to meet specified performance from
0°C to 70°C and is designed, characterized and expected to meet these
extended temperature limits, but is not tested at –40°C and 85°C. The
LT1610I is guaranteed to meet the extended temperature limits.
Note 3: Current limit guaranteed by design and/or correlation to static test.
Current limit is affected by duty cycle due to ramp generator. See Block
Diagram.
Note 4: Not 100% tested at 85°C.
3
LT1610
UW
TYPICAL PERFOR A CE CHARACTERISTICS
Current Limit (DC = 30%)
600
500
400
(mV)
CESAT
300
V
200
100
CESAT
0
vs Current
TA = 25°C
200300400
100
SWITCH CURRENT (mA)
TA = 85°C
= –40°C
T
A
500600
1610 G01
vs Temperature
800
700
600
500
400
SWITCH CURRENT LIMIT (mA)
300
200
–50
02550
–25
TEMPERATURE (°C)
75100
1610 G02
Current Limit vs Duty CycleV
800
700
600
500
400
300
CURRENT LIMIT (mA)
200
100
0
2040601007010305090
0
TA = 25°C
80
DUTY CYCLE (%)
1610 G03
Oscillator Frequency
vs Input VoltageFeedback Voltage
2.50
TA = 25°C
2.25
2.00
1.75
1.50
1.25
1.00
0.75
0.50
SWITCHING FREQUENCY (MHz)
0.25
0
0
13
2
INPUT VOLTAGE (V)
SHDN Pin Current
vs SHDN Pin Voltage
50
40
30
20
SHDN CURRENT (µA)
10
7
4
6
5
1610 G04
1.240
1.235
1.230
1.225
1.220
FEEDBACK VOLTAGE (V)
1.215
1.210
8
V
OUT
50mV/DIV
AC COUPLED
100mA/DIV
31mA
I
LOAD
1mA
–50
–25
Transient Response,
Circuit of Figure 1
I
L1
VIN = 1.25V500µs/DIV
V
= 3V
OUT
02550
TEMPERATURE (°C)
75100
1610 G05
1610 TA08
40
35
30
25
20
15
10
QUIESCENT CURRENT (µA)
V
OUT
20mV/DIV
AC COUPLED
SWITCH
VOLTAGE
2V/DIV
SWITCH
CURRENT
50mA/DIV
Quiescent Current
vs Temperature
5
0
–25050
–50
25
TEMPERATURE (°C)
Burst Mode Operation,
Circuit of Figure 1
= 1.25V20µs/DIV
V
IN
= 3V
V
OUT
= 3mA
I
LOAD
75
100
1610 G06
1610 TA08
4
0
0
12
SHDN VOLTAGE (V)
4
358
67
1610 G07
UUU
PIN FUNCTIONS
LT1610
VC (Pin 1): Error Amplifier Output. Frequency compensation network must be connected to this pin, either internal
(COMP pin) or external series RC to ground. 220kΩ/
220pF typical value.
FB (Pin 2): Feedback Pin. Reference voltage is 1.23V.
Connect resistive divider tap here. Minimize trace area at
FB. Set V
according to V
OUT
= 1.23V (1 + R1/R2).
OUT
SHDN (Pin 3): Shutdown. Ground this pin to turn off
device. Tie to 1V or more to enable.
PGND (Pin 4): Power Ground. Tie directly to local ground
plane.
W
BLOCK DIAGRA
V
IN
V
OUT
R1
(EXTERNAL)
R2
(EXTERNAL)
6
R5
40k
Q1
FB
2
FB
Q2
× 10
R6
40k
R3
30k
V
IN
+
A1
g
m
–
SW (Pin 5): Switch Pin. Connect inductor/diode here.
Minimize trace area at this pin to keep EMI down.
VIN (Pin 6): Input Supply Pin. Must be locally bypassed.
GND (Pin 7): Signal Ground. Carries all device ground
current except switch current. Tie to local ground plane.
COMP (Pin 8): Internal Compensation Network. Tie to V
C
pin, or let float if external compensation is used. Output
capacitor must be tantalum if COMP pin is used for compensation.
1
V
C
COMP
8
R
C
C
C
3
SHDNSHUTDOWN
GND
7
R4
140k
+
BIAS
RAMP
GENERATOR
Σ
1.7MHz
OSCILLATOR
–
A2
+
–
COMPARATOR
Figure 2. LT1610 Block Diagram
ENABLE
FF
RQ
S
A = 3
DRIVER
+
–
5
Q3
4
SW
0.15Ω
PGND
1610 F02
5
LT1610
U
WUU
APPLICATIONS INFORMATION
OPERATION
The LT1610 combines a current mode, fixed frequency
PWM architecture with Burst Mode micropower operation
to maintain high efficiency at light loads. Operation can be
best understood by referring to the block diagram in
Figure 2. Q1 and Q2 form a bandgap reference core whose
loop is closed around the output of the converter. When
VIN is 1V, the feedback voltage of 1.23V, along with an
70mV drop across R5 and R6, forward biases Q1 and Q2’s
base collector junctions to 300mV. Because this is not
enough to saturate either transistor, FB can be at a higher
voltage than VIN. When there is no load, FB rises slightly
above 1.23V, causing VC (the error amplifier’s output) to
decrease. When VC reaches the bias voltage on hysteretic
comparator A1, A1’s output goes low, turning off all
circuitry except the input stage, error amplifier and lowbattery detector. Total current consumption in this state is
30µA. As output loading causes the FB voltage to de-
crease, A1’s output goes high, enabling the rest of the IC.
Switch current is limited to approximately 100mA initially
after A1’s output goes high. If the load is light, the output
voltage (and FB voltage) will increase until A1’s output
goes low, turning off the rest of the LT1610. Low frequency ripple voltage appears at the output. The ripple
frequency is dependent on load current and output capacitance. This Burst Mode operation keeps the output regulated and reduces average current into the IC, resulting in
high efficiency even at load currents of 1mA or less.
If the output load increases sufficiently, A1’s output remains
high, resulting in continuous operation. When the LT1610
is running continuously, peak switch current is controlled
by VC to regulate the output voltage. The switch is turned
on at the beginning of each switch cycle. When the summation of a signal representing switch current and a ramp
generator (introduced to avoid subharmonic oscillations at
duty factors greater than 50%) exceeds the VC signal,
comparator A2 changes state, resetting the flip-flop and
turning off the switch. Output voltage increases as switch
current is increased. The output, attenuated by a resistor
divider, appears at the FB pin, closing the overall loop.
Frequency compensation is provided by either an external
series RC network connected between the VC pin and
ground or the internal RC network on the COMP pin (Pin
8). The typical values for the internal RC are 50k and 50pF.
LAYOUT
Although the LT1610 is a relatively low current device, its
high switching speed mandates careful attention to layout
for optimum performance. For boost converters, follow
the component placement indicated in Figure 3 for the best
results. C2’s negative terminal should be placed close to
Pin 4 of the LT1610. Doing this reduces switching currents
in the ground copper which keeps high frequency “spike”
noise to a minimum. Tie the local ground into the system
ground plane at one point only, using a few vias, to avoid
introducing dI/dt induced noise into the ground plane.
6
GROUND PLANE
R1
SHUTDOWN
MULTIPLE
VIAs
Figure 3. Recommended Component Placement for Boost Converter. Note Direct High Current Paths Using
Wide PC Traces. Minimize Trace Area at Pin 1 (VC) and Pin 2 (FB). Use Multiple Vias to Tie Pin 4 Copper to
Ground Plane. Use Vias at One Location Only to Avoid Introducing Switching Currents into the Ground Plane
R2
GND
1
2
LT1610
3
4
+
C2
8
C1
7
6
5
D1
V
OUT
V
IN
+
L1
1610 F03
LT1610
U
WUU
APPLICATIONS INFORMATION
A SEPIC (Single-Ended Primary Inductance Converter)
schematic is shown in Figure 4. This converter topology
produces a regulated output over an input voltage range
that spans (i.e., can be higher or lower than) the output.
Recommended component placement for a SEPIC is
shown in Figure 5.
C3
1µF
•
SW
SHDN
PGND
CERAMIC
2
FB
3
4
SHUTDOWN
1M
604k
•
L2
22µH
D1
V
OUT
3.3V
120mA
+
C2
22µF
6.3V
1610 F04
GROUND PLANE
R1
R2
SHUTDOWN
MULTIPLE
VIAs
Figure 4. Li-Ion to 3.3V SEPIC DC/DC Converter
V
IN
1
2
LT1610
3
4
C2
8
C1
7
6
5
+
L1L2
C3
+
GND
D1
V
OUT
1610 F05
Figure 5. Recommended Component Placement for SEPIC
7
LT1610
U
WUU
APPLICATIONS INFORMATION
COMPONENT SELECTION
Inductors
Inductors used with the LT1610 should have a saturation
current rating (–30% of zero current inductance) of approximately 0.5A or greater. DCR should be 0.5Ω or less.
The value of the inductor should be matched to the power
requirements and operating voltages of the application. In
most cases a value of 4.7µH or 10µH is suitable. The Murata
LQH3C inductors specified throughout the data sheet are
small and inexpensive, and are a good fit for the LT1610.
Alternatives are the CD43 series from Sumida and the
DO1608 series from Coilcraft. These inductors are slightly
larger but will result in slightly higher circuit efficiency.
Chip inductors, although tempting to use because of their
small size and low cost, generally do not have enough
energy storage capacity or low enough DCR to be used
successfully with the LT1610.
Diodes
The Motorola MBR0520 is a 0.5 amp, 20V Schottky diode.
This is a good choice for nearly any LT1610 application,
unless the output voltage or the circuit topology require a
diode rated for higher reverse voltages. Motorola also
offers the MBR0530 (30V) and MBR0540 (40V) versions.
Most one-half amp and one amp Schottky diodes are
suitable; these are available from many manufacturers. If
you use a silicon diode, it must be an ultrafast recovery
type. Efficiency will be lower due to the silicon diode’s
higher forward voltage drop.
Capacitors
impedance of the output capacitor. The capacitor should
have low impedance at the 1.7MHz switching frequency of
the LT1610. At this frequency, the impedance is usually
dominated by the capacitor’s equivalent series resistance
(ESR). Choosing a capacitor with lower ESR will result in
lower output ripple.
Perhaps the best way to decrease ripple is to add a 1µF
ceramic capacitor in parallel with the bulk output capacitor. Ceramic capacitors have very low ESR and 1µF is
enough capacitance to result in low impedance at the
switching frequency. The low impedance can have a
dramatic effect on output ripple voltage. To illustrate,
examine Figure 6’s circuit, a 4-cell to 5V/100mA SEPIC
DC/DC converter. This design uses inexpensive aluminum
electrolytic capacitors at input and output to keep cost
down. Figure 7 details converter operation at a 100mA
load, without ceramic capacitor C5. Note the 400mV
spikes on V
After C5 is installed, output ripple decreases by a factor of
8 to about 50mV
efficiency by 1 to 2 percent.
Low ESR and the required bulk output capacitance can be
obtained using a single larger output capacitor. Larger
tantalum capacitors, newer capacitor technologies (for
example the POSCAP from Sanyo and SPCAP from
Panasonic) or large value ceramic capacitors will reduce
the output ripple. Note, however, that the stability of the
circuit depends on both the value of the output capacitor
and its ESR. When using low value capacitors or capacitors with very low ESR, circuit stability should be evaluated carefully, as described below.
OUT
.
. The addition of C5 also improves
P-P
The input capacitor must be placed physically close to the
LT1610. ESR is not critical for the input. In most cases
inexpensive tantalum can be used.
The choice of output capacitor is far more important. The
quality of this capacitor is the greatest determinant of the
output voltage ripple. The output capacitor performs two
major functions. It must have enough capacitance to
satisfy the load under transient conditions and it must
shunt the AC component of the current coming through
the diode from the inductor. The ripple on the output
results when this AC current passes through the finite
8
Loop Compensation
The LT1610 is a current mode PWM switching regulator
that achieves regulation with a linear control loop. The
LT1610 provides the designer with two methods of compensating this loop. First, you can use an internal compensation network by tying the COMP pin to the VC pin. This
results in a very small solution and reduces the circuit’s
total part count. The second option is to tie a resistor R
and a capacitor CC in series from the VC pin to ground. This
allows optimization of the transient response for a wide
variety of operating conditions and power components.
C
LT1610
U
WUU
APPLICATIONS INFORMATION
+
V
OUT
200mV/DIV
I
DIODE
500mA/DIV
4 CELLS
C1
22µF
6.3V
C1, C2: ALUMINUM ELECTROLYTIC
C3 TO C5: CERAMIC X7R OR X5R
D1: MBR0520
L1, L2: MURATA LQH3C220 OR SUMIDA CLS62-220
Figure 6. 4-Cell Alkaline to 5V/120mA SEPIC DC/DC Converter
C4
1µF
CERAMIC
L1
22µH
65
V
IN
1
V
C
LT1610
8
COMP
GND
7
C3
1µF
•
SW
SHDN
PGND
CERAMIC
2
FB
3
4
SHUTDOWN
1M
324k
•
D1
L2
22µH
V
OUT
5V
120mA
+
C2
22µF
6.3V
1610 F06
C5
1µF
CERAMIC
sation network is modified to achieve stable operation.
Linear Technology’s Application Note 19 contains a detailed description of the method. A good starting point for
the LT1610 is CC ~ 220pF and RC ~ 220k.
SWITCH
VOLTAGE
10V/DIV
100ns/DIV
1610 F07
Figure 7. Switching Waveforms Without Ceramic Capacitor C5
V
OUT
50mV/DIV
I
DIODE
500mA/DIV
SWITCH
VOLTAGE
10V/DIV
= 4.1V100ns/DIV1610 F08
V
IN
LOAD = 100mA
Figure 8. Switching Waveforms with Ceramic Capacitor C5.
Note the 50mV/DIV Scale for V
OUT
It is best to choose the compensation components empirically. Once the power components have been chosen
(based on size, efficiency, cost and space requirements),
a working circuit is built using conservative (or merely
guessed) values of RC and CC. Then the response of the
circuit is observed under a transient load, and the compen-
All Ceramic, Low Profile Design
Large value ceramic capacitors that are suitable for use as
the main output capacitor of an LT1610 regulator are now
available. These capacitors have very low ESR and therefore offer very low output ripple in a small package.
However, you should approach their use with some
caution.
Ceramic capacitors are manufactured using a number of
dielectrics, each with different behavior across temperature and applied voltage. Y5V is a common dielectric used
for high value capacitors, but it can lose more than 80% of
the original capacitance with applied voltage and extreme
temperatures. The transient behavior and loop stability of
the switching regulator depend on the value of the output
capacitor, so you may not be able to afford this loss. Other
dielectrics (X7R and X5R) result in more stable characteristics and are suitable for use as the output capacitor. The
X7R type has better stability across temperature, whereas
the X5R is less expensive and is available in higher values.
The second concern in using ceramic capacitors is that
many switching regulators benefit from the ESR of the
9
LT1610
U
WUU
APPLICATIONS INFORMATION
output capacitor because it introduces a zero in the
regulator’s loop gain. This zero may not be effective
because the ceramic capacitor’s ESR is very low. Most
current mode switching regulators (including the LT1610)
can easily be compensated without this zero. Any design
should be tested for stability at the extremes of operating
temperatures; this is particularly so of circuits that use
ceramic output capacitors.
Figure 9 details a 2.5V to 5V boost converter. Transient
response to a 5mA to 105mA load step is pictured in Figure
10. The “double trace” of V
ESR of C2. This ESR aids stability. In Figure 11, C2 is
replaced by a 10µF ceramic capacitor. Note the low phase
margin; at higher input voltage, the converter may oscillate. After replacing the internal compensation network
with an external 220pF/220k series RC, the transient
response is shown in Figure 12. This is acceptable transient response.