7
LT1956/LT1956-5
1956f
it much easier to frequency compensate the feedback loop
and also gives much quicker transient response.
Most of the circuitry of the LT1956 operates from an
internal 2.9V bias line. The bias regulator normally draws
power from the regulator input pin, but if the BIAS pin is
connected to an external voltage higher than 3V, bias
power will be drawn from the external source (typically the
regulated output voltage). This will improve efficiency if
the BIAS pin voltage is lower than regulator input voltage.
High switch efficiency is attained by using the BOOST pin
to provide a voltage to the switch driver which is higher
than the input voltage, allowing switch to be saturated.
This boosted voltage is generated with an external capaci-
tor and diode. Two comparators are connected to the
shutdown pin. One has a 2.38V threshold for undervoltage
lockout and the second has a 0.4V threshold for complete
shutdown.
The LT1956 is a constant frequency, current mode buck
converter. This means that there is an internal clock and
two feedback loops that control the duty cycle of the power
switch. In addition to the normal error amplifier, there is a
current sense amplifier that monitors switch current on a
cycle-by-cycle basis. A switch cycle starts with an oscilla-
tor pulse which sets the R
S
flip-flop to turn the switch on.
When switch current reaches a level set by the inverting
input of the comparator, the flip-flop is reset and the
switch turns off. Output voltage control is obtained by
using the output of the error amplifier to set the switch
current trip point. This technique means that the error
amplifier commands current to be delivered to the output
rather than voltage. A voltage fed system will have low
phase shift up to the resonant frequency of the inductor
and output capacitor, then an abrupt 180° shift will occur.
The current fed system will have 90° phase shift at a much
lower frequency, but will not have the additional 90° shift
until well beyond the LC resonant frequency. This makes
BLOCK DIAGRA
W
Figure 1. LT1956 Block Diagram
+
+
+
+
Σ
V
IN
2.9V BIAS
REGULATOR
500kHz
OSCILLATOR
FREQUENCY
FOLDBACK
SW
FB
GND
1, 8, 9, 16
1956 F01
SLOPE COMP
ANTISLOPE COMP
BIAS
INTERNAL
V
CC
SYNC
0.4V
5.5µA
CURRENT
COMPARATOR
R
LIMIT
R
SENSE
ERROR
AMPLIFIER
g
m
= 2000µMho
Q2
FOLDBACK
CURRENT
LIMIT
CLAMP
BOOST
R
S
FLIP-FLOP
DRIVER
CIRCUITRY
S
R
Q1
POWER
SWITCH
1.22V
4
10
14
SHDN
15
6
2
12
11
V
C
LOCKOUT
COMPARATOR
SHUTDOWN
COMPARATOR
2.38V
×1
Q3
V
C(MAX)
CLAMP
8
LT1956/LT1956-5
1956f
current through the diode and inductor is equal to the
short-circuit current limit of the switch (typically 2A for
the LT1956, folding back to less than 1A). Minimum
switch on time limitations would prevent the switcher
from attaining a sufficiently low duty cycle if switching
frequency were maintained at 500kHz, so frequency is
reduced by about 5:1 when the feedback pin voltage drops
below 0.8V (see Frequency Foldback graph). This does
not affect operation with normal load conditions; one
simply sees a shift in switching frequency during start-up
as the output voltage rises.
In addition to lower switching frequency, the LT1956 also
operates at lower switch current limit when the feedback
pin voltage drops below 0.6V. Q2 in Figure 2 performs this
function by clamping the V
C
pin to a voltage less than its
normal 2.1V upper clamp level. This
foldback current limit
greatly reduces power dissipation in the IC, diode and in-
ductor during short-circuit conditions. External synchro-
nization is also disabled to prevent interference with fold-
back operation. Again, it is nearly transparent to the user
under normal load conditions. The only loads that may be
affected are current source loads which maintain full load
current with output voltage less than 50% of final value. In
these rare situations the feedback pin can be clamped above
0.6V with an external diode to defeat foldback current limit.
Caution:
clamping the feedback pin means that frequency
shifting will also be defeated, so a combination of high in-
put voltage and dead shorted output may cause the LT1956
to lose control of current limit.
The internal circuitry which forces reduced switching
frequency also causes current to flow out of the feedback
pin when output voltage is low. The equivalent circuitry is
shown in Figure 2. Q1 is completely off during normal
operation. If the FB pin falls below 0.8V, Q1 begins to
conduct current and reduces frequency at the rate of
approximately 3.5kHz/µA. To ensure adequate frequency
foldback (under worst-case short-circuit conditions), the
external divider Thevinin resistance must be low enough
to pull 115µA out of the FB pin with 0.44V on the pin (R
DIV
3.8k).
The net result is that reductions in frequency and
current limit are affected by output voltage divider imped-
ance. Although divider impedance is not critical, caution
should be used if resistors are increased beyond the
suggested values and short-circuit conditions will occur
FEEDBACK PIN FUNCTIONS
The feedback (FB) pin on the LT1956 is used to set output
voltage and provide several overload protection features.
The first part of this section deals with selecting resistors
to set output voltage and the remaining part talks about
foldback frequency and current limiting created by the FB
pin. Please read both parts before committing to a final
design. The 5V fixed output voltage part (LT1956-5) has
internal divider resistors and the FB pin is renamed SENSE,
connected directly to the output.
The suggested value for the output divider resistor (see
Figure 2) from FB to ground (R2) is 5k or less, and a
formula for R1 is shown below. The output voltage error
caused by ignoring the input bias current on the FB pin is
less than 0.25% with R2 = 5k. A table of standard 1%
values is shown in Table 1 for common output voltages.
Please read the following section if divider resistors are
increased above the suggested values.
R
RV
OUT
1
2122
122
=
()
.
.
Table 1
OUTPUT R1 % ERROR AT OUTPUT
VOLTAGE R2 (NEAREST 1%) DUE TO DISCRETE 1%
(V) (k
)(k
) RESISTOR STEPS
3 4.99 7.32 +0.32
3.3 4.99 8.45 0.43
5 4.99 15.4 0.30
6 4.75 18.7 +0.38
8 4.47 24.9 +0.20
10 4.32 30.9 0.54
12 4.12 36.5 +0.24
15 4.12 46.4 0.27
More Than Just Voltage Feedback
The feedback pin is used for more than just output voltage
sensing. It also reduces switching frequency and current
limit when output voltage is very low (see the Frequency
Foldback graph in Typical Performance Characteristics).
This is done to control power dissipation in both the IC
and in the external diode and inductor during short-circuit
conditions. A shorted output requires the switching regu-
lator to operate at very low duty cycles, and the average
APPLICATIO S I FOR ATIO
WUUU
9
LT1956/LT1956-5
1956f
Figure 2. Frequency and Current Limit Foldback
with high input voltage.
High frequency pickup will in-
crease and the protection accorded by frequency and
current foldback will decrease.
CHOOSING THE INDUCTOR
For most applications, the output inductor will fall into the
range of 5µH to 30µH. Lower values are chosen to reduce
physical size of the inductor. Higher values allow more
output current because they reduce peak current seen by
the LT1956 switch, which has a 1.5A limit. Higher values
also reduce output ripple voltage.
When choosing an inductor you will need to consider
output ripple voltage, maximum load current, peak induc-
tor current and fault current in the inductor. In addition,
other factors such as core and copper losses, allowable
component height, EMI, saturation and cost should also
be considered. The following procedure is suggested as a
way of handling these somewhat complicated and con-
flicting requirements.
Output Ripple Voltage
Figure 3 shows a comparison of output ripple voltage for
the LT1956 using either a tantalum or ceramic output
capacitor. It can be seen from Figure 3 that output ripple
voltage can be significantly reduced by using the ceramic
output capacitor; the significant decrease in output ripple
voltage is due to the very low ESR of ceramic capacitors.
+
1.2V
BUFFER
V
SW
L1
V
C
GND
TO SYNC CIRCUIT
1956 F02
TO FREQUENCY
SHIFTING
R3
1k
R4
2k
R1
C1
R2
OUTPUT
5V
ERROR
AMPLIFIER
FB
1.4V
Q1
LT1956
Q2
+
APPLICATIO S I FOR ATIO
WUUU
Output ripple voltage is determined by ripple current
(I
LP-P
) through the inductor and the high frequency
impedance of the output capacitor. At high frequencies,
the impedance of the tantalum capacitor is dominated by
its effective series resistance (ESR).
Tantalum Output Capacitor
The typical method for reducing output ripple voltage
when using a tantalum output capacitor is to increase the
inductor value (to reduce the ripple current in the induc-
tor). The following equations will help in choosing the
required inductor value to achieve a desirable output ripple
voltage level. If output ripple voltage is of less importance,
the subsequent suggestions in Peak Inductor and Fault
Current and EMI will additionally help in the
selection of
the inductor value.
Figure 3. LT1956 Output Ripple Voltage Waveforms.
Ceramic vs Tantalum Output Capacitors
1µs/DIV
10mV/DIV
V
OUT
USING
22µF CERAMIC
OUTPUT
CAPACITOR
V
OUT
USING
100µF, 0.08
TANTALUM
OUTPUT
CAPACITOR
10mV/DIV
V
IN
= 12V
V
OUT
= 5V
L = 15µH
1956 F03

LT1956IFE#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Hi V, 1.5A, 500kHz Buck Sw Regs
Lifecycle:
New from this manufacturer.
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