LT1110
10
Diode Selection
Speed, forward drop, and leakage current are the three
main considerations in selecting a catch diode for LT1110
converters. General purpose rectifiers such as the 1N4001
are
unsuitable
for use in
any
switching regulator applica-
tion. Although they are rated at 1A, the switching time of
a 1N4001 is in the 10µs-50µs range. At best, efficiency will
be severely compromised when these diodes are used; at
worst, the circuit may not work at all. Most LT1110 circuits
will be well served by a 1N5818 Schottky diode, or its
surface mount equivalent, the MBRS130T3. The combina-
tion of 500mV forward drop at 1A current, fast turn ON and
turn OFF time, and 4µA to 10µA leakage current fit nicely
with LT1110 requirements. At peak switch currents of
100mA or less, a 1N4148 signal diode may be used. This
diode has leakage current in the 1nA-5nA range at 25°C
and lower cost than a 1N5818. (You can also use them to
get your circuit up and running, but beware of destroying
the diode at 1A switch currents.)
Step-Up (Boost Mode) Operation
A step-up DC-DC converter delivers an output voltage
higher than the input voltage. Step-up converters are
not
short circuit protected since there is a DC path from input
to output.
The usual step-up configuration for the LT1110 is shown
in Figure 4. The LT1110 first pulls SW1 low causing V
IN
V
CESAT
to appear across L1. A current then builds up in L1.
At the end of the switch ON time the current in L1 is
1
:
I
V
L
t
PEAK
IN
ON
= ()20
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Immediately after switch turn off, the SW1 voltage pin
starts to rise because current cannot instantaneously stop
flowing in L1. When the voltage reaches V
OUT
+ V
D
, the
inductor current flows through D1 into C1, increasing
V
OUT
. This action is repeated as needed by the LT1110 to
keep V
FB
at the internal reference voltage of 220mV. R1
and R2 set the output voltage according to the formula
V
R
R
mV
OUT
=+
()
1
2
1
220 21.()
Step-Down (Buck Mode) Operation
A step-down DC-DC converter converts a higher voltage
to a lower voltage. The usual hookup for an LT1110 based
step-down converter is shown in Figure 5.
LT1110 • TA15
GND
SW2
SW1
LIM
I
IN
V
R3
220
FB
V
OUT
+
C2
+
C1
D1
1N5818
V
IN
R2
R1
L1
LT1110
Figure 5. Step-Down Mode Hookup
When the switch turns on, SW2 pulls up to V
IN
– V
SW
. This
puts a voltage across L1 equal to V
IN
– V
SW
– V
OUT
,
causing a current to build up in L1. At the end of the switch
ON time, the current in L1 is equal to
I
V
VV
L
t
PEAK
IN
SW OUT
ON
=
−−
.()22
When the switch turns off, the SW2 pin falls rapidly and
actually goes below ground. D1 turns on when SW2
reaches 0.4V below ground.
D1
MUST BE A SCHOTTKY
DIODE
. The voltage at SW2 must never be allowed to go
below –0.5V. A silicon diode such as the 1N4933 will allow
SW2 to go to –0.8V, causing potentially destructive power
Figure 4. Step-Up Mode Hookup.
L1
LT1110 • TA14
GND SW2
SW1
LIM
I
IN
V
D1
R3*
LT1110
+
V
OUT
R2
R1
C1
* = OPTIONAL
V
IN
FB
Note 1: This simple expression neglects the effects of switch and coil
resistance. This is taken into account in the “Inductor Selection” section.
LT1110
11
Converter” section with the following conservative ex-
pression for V
SW
:
VVV V
SW R SAT
=+
1
09 24.. ()
R2 provides a current path to turn off Q1. R3 provides base
drive to Q1. R4 and R5 set output voltage.
Inverting Configurations
The LT1110 can be configured as a positive-to-negative
converter (Figure 7), or a negative-to-positive converter
(Figure 8). In Figure 7, the arrangement is very similar to
a step-down, except that the high side of the feedback is
referred to ground. This level shifts the output negative. As
in the step-down mode, D1 must be a Schottky diode,
andV
OUT
should be less than 6.2V. More negative out-
put voltages can be accommodated as in the prior section.
LT1110 • TA03
–V
OUT
+
C2
+
C1
D1
1N5818
+V
IN
R1
R2
L1
GND
SW2
SW1
LIM
I
IN
V
R3
FB
LT1110
Figure 7. Positive-to-Negative Converter
In Figure 8, the input is negative while the output is
positive. In this configuration, the magnitude of the input
voltage can be higher or lower than the output voltage. A
level shift, provided by the PNP transistor, supplies proper
polarity feedback information to the regulator.
dissipation inside the LT1110. Output voltage is deter-
mined by
V
R
R
mV
OUT
=+
()
1
2
1
220 23.()
R3 programs switch current limit. This is especially im-
portant in applications where the input varies over a wide
range. Without R3, the switch stays on for a fixed time
each cycle. Under certain conditions the current in L1 can
build up to excessive levels, exceeding the switch rating
and/or saturating the inductor. The 220 resistor pro-
grams the switch to turn off when the current reaches
approximately 800mA. When using the LT1110 in step-
down mode, output voltage should be limited to 6.2V or
less. Higher output voltages can be accommodated by
inserting a 1N5818 diode in series with the SW2 pin
(anode connected to SW2).
Higher Current Step-Down Operation
Output current can be increased by using a discrete PNP
pass transistor as shown in Figure 6. R1 serves as a
current limit sense. When the voltage drop across R1
equals a V
BE
, the switch turns off. For temperature com-
pensation a Schottky diode can be inserted in series with
the I
LIM
pin. This also lowers the maximum drop across R1
to V
BE
– V
D
, increasing efficiency. As shown, switch
current is limited to 2A. Inductor value can be calculated
based on formulas in the “Inductor Selection Step-Down
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Figure 6. Q1 Permits Higher-Current Switching.
LT1110 Functions as Controller.
LT1110 • TA16
D1
1N5821
+
+
V
OUT
V
IN
25V
MAX
L1
R1
0.3
R2
220
Q1
MJE210 OR
ZETEX ZTX789A
R3
330
R4
R5
C1
V
OUT
= 220mV
(
1 +
)
R4
R5
LT1110
GND
SW2
SW1
V
IN
I
L
FB
C2
Figure 8. Negative-to-Positive Converter
L1
LT1110 • TA04
GND SW2
FB
SW1
LIM
I
IN
V
D1
AO
+V
OUT
R2
V
OUT
= 220mV + 0.6V
R1
R2
( )
R1
2N3906
–V
IN
+
C1
LT1110
+
C2
LT1110
12
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Using the I
LIM
Pin
The LT1110 switch can be programmed to turn off at a set
switch current, a feature not found on competing devices.
This enables the input to vary over a wide range without
exceeding the maximum switch rating or saturating the
inductor. Consider the case where analysis shows the
LT1110 must operate at an 800mA peak switch current
with a 2.0V input. If V
IN
rises to 4V, peak current will rise
to 1.6A, exceeding the maximum switch current rating.
With the proper resistor selected (see the “Maximum
Switch
Current vs R
LIM
” characteristic), the switch current
will be limited to 800mA, even if the input voltage
increases.
Another situation where the I
LIM
feature is useful occurs
when the device goes into continuous mode operation.
This occurs in step-up mode when
V
V
VV DC
OUT DIODE
IN SW
+
<
1
1
25.()
When the input and output voltages satisfy this relation-
ship, inductor current does not go to zero during the
switch OFF time. When the switch turns on again, the
current ramp starts from the non-zero current level in the
inductor just prior to switch turn on. As shown in Figure 9,
the inductor current increases to a high level before the
comparator turns off the oscillator. This high current can
cause excessive output ripple and requires oversizing the
output capacitor and inductor. With the I
LIM
feature,
however, the switch current turns off at a programmed
level as shown in Figure 10, keeping output ripple to a
minimum.
Figure 11 details current limit circuitry. Sense transistor
Q1, whose base and emitter are paralleled with power
switch Q2, is ratioed such that approximately 0.5% of Q2’s
collector current flows in Q1’s collector. This current is
passed through internal 80 resistor R1 and out through
the I
LIM
pin. The value of the external resistor connected
between I
LIM
and V
IN
set the current limit. When sufficient
switch current flows to develop a V
BE
across R1 + R
LIM
, Q3
turns on and injects current into the oscillator, turning off
the switch. Delay through this circuitry is approximately
800ns. The current trip point becomes less accurate for
switch ON times less than 3µs. Resistor values program-
ming switch ON time for 800ns or less will cause spurious
response in the switch circuitry although the device will
still maintain output regulation.
LT1110 • TA05
I
OFF
L
ON
SWITCH
Figure 9. No Current Limit Causes Large Inductor
Current Build-Up
LT1110 • TA06
I
ON
L
OFF
SWITCH
PROGRAMMED CURRENT LIMIT
Figure 10. Current Limit Keeps Inductor Current Under Control
LT1110 • TA17
SW2
SW1
Q2
DRIVER
OSCILLATOR
V
IN
I
LIM
R1
80
(INTERNAL)
R
LIM
(EXTERNAL)
Q1
Q3
Figure 11. LT1110 Current Limit Circuitry
Using the Gain Block
The gain block (GB) on the LT1110 can be used as an error
amplifier, low battery detector or linear post regulator. The
gain block itself is a very simple PNP input op amp with an
open collector NPN output. The negative input of the gain
block is tied internally to the 220mV reference. The posi-
tive input comes out on the SET pin.

LT1110CN8#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Micropower DC-DC Converter Adjustable and Fixed 5V, 12V
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