LTC1704/LTC1704B
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is the same as the output current. The LTC1704 current
limit circuit inverts the voltage at I
MAX
before comparing
it with the negative voltage across QB, allowing the current
limit to be set with a positive voltage.
To set the current limit, calculate the expected voltage
drop across QB at the maximum desired current:
V
PROG
= (I
LIMIT
)(R
DS(ON)
)
I
LIMIT
should be chosen to be quite a bit higher than the
expected operating current, to allow for MOSFET R
DS(ON)
changes with temperature. Setting I
LIMIT
to 150% of the
maximum normal operating current is usually safe and will
adequately protect the power components if they are
chosen properly. Note that the ringing on the switch node
can cause error for the current limit threshold (illustrated
in Figure 6). This factor will change depending on the
layout and the components used. V
PROG
is then pro-
grammed at the I
MAX
pin using the internal 10µA pull-up
and an external resistor:
R
IMAX
= V
PROG
/10µA
The resulting value of R
IMAX
should be checked in an ac-
tual circuit to ensure that the current circuit kicks in as
expected. MOSFET R
DS(ON)
specs are like horsepower
ratings in automobiles, and should be taken with a grain of
salt. Circuits that use very low values for R
IMAX
(<10k)
should be checked carefully, since small changes in R
IMAX
can cause large I
LIMIT
changes when the switch node ring-
ing makes up a large percentage of the total V
PROG
value.
If V
PROG
is set too low, the LTC1704 may fail to start up.
Accuracy Trade-Offs
The V
DS
sensing scheme used in the LTC1704 is not
particularly accurate, primarily due to uncertainty in the
R
DS(ON)
from MOSFET to MOSFET. A second error term
arises from the ringing present at the SW pin, which
causes the V
DS
to look larger than (I
LOAD
)(R
DS(ON)
) at the
beginning of QB’s on-time. Another important error is due
to poor PCB layout. Care should be taken to ensure that
proper kelvin sensing of the SW pin is provided. These
inaccuracies do not prevent the LTC1704 current limit
circuit from protecting itself and the load from damaging
overcurrent conditions, but they do prevent the user from
setting the current limit to a tight tolerance if more than
one copy of the circuit is being built. The 50% factor in the
current setting equation above reflects the margin neces-
sary to ensure that the circuit will stay out of current limit
at the maximum normal load, even with a hot MOSFET that
is running quite a bit higher than its R
DS(ON)
spec.
REGULATION OVER COMPONENT
TOLERANCE/TEMPERATURE
DC Regulation Accuracy
The LTC1704’s switcher controller initial DC output accu-
racy depends mainly on internal reference accuracy and
internal op amp offset. Two LTC1704 specs come into
play: feedback voltage and feedback voltage line regula-
tion. The feedback voltage spec is 800mV ±12mV over the
full temperature range and is specified at the FB pin, which
encompasses both reference accuracy and any op amp
offset. This accounts for 1.5% error at the output with a 5V
input supply. The feedback voltage line regulation spec
adds an additional 0.1%/V term that accounts for change
in reference output with change in input supply voltage.
With a 5V supply, the errors contributed by the LTC1704
itself add up to no more than 1.5% DC error at the output.
The output voltage setting resistors (see R1 and R2 in the
Typical Applications) are the other major contributor to DC
error. At a typical 1.xV output voltage, the resistors are of
roughly the same value, which tends to halve their error
terms, improving accuracy. Still, using 1% resistors for
R1 and R2 will add 1% to the total output error budget.
Using 0.1% resistors in just those two positions can nearly
halve the DC output error for very little additional cost.
Load Regulation
Load regulation is affected by feedback voltage, feedback
amplifier gain and external ground drops in the feedback
path. Feedback voltage is covered above and is within
1.5% over temperature. A full range load step might
require a 10% duty cycle change to keep the output
constant, requiring the COMP pin to move about 100mV.
With amplifier gain at 85dB, this adds up to only a 10µV
shift at FB, negligible compared to the reference accuracy
terms.
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External ground drops aren’t so negligible. The LTC1704
can sense the positive end of the output voltage by
attaching the feedback resistor directly at the load, but it
cannot do the same with the ground lead. Just 0.001 of
resistance in the ground lead at 10A load will cause a 10mV
error in the output voltage—as much as all the other DC
errors put together. Proper layout becomes essential to
achieving optimum load regulation from the LTC1704. A
properly laid out LTC1704 circuit should move less than a
millivolt at the output from zero to full load.
Transient Response
Transient response is the other half of the regulation
equation. The LTC1704 can keep the DC output voltage
constant to within 1% when averaged over hundreds of
cycles. Over just a few cycles, however, the external
components conspire to limit the speed that the output
can move. Consider a typical 5V to 1.5V circuit, subjected
to a 1A to 5A load transient. Initially, the loop is in
regulation and the DC current in the output capacitor is
zero. Suddenly, an extra 4A start flowing out of the output
capacitor while the inductor is still supplying only 1A. This
sudden change will generate a (4A)(R
ESR
) voltage step at
the output; with a typical 0.015 output capacitor ESR,
this is a 60mV step at the output, or 4% (for a 1.5V output
voltage.)
Very quickly, the feedback loop will realize that something
has changed and will move at the bandwidth allowed by
the external compensation network towards a new duty
cycle. If the bandwidth is set to 50kHz, the COMP pin will
get to 60% of the way to 90% duty cycle in 3µs. Now the
inductor is seeing 3.5V across itself for a large portion of
the cycle, and its current will increase from 1A at a rate set
by di/dt = V/L. If the inductor value is 0.5µH, the di/dt will
be 3.5V/0.5µH or 7A/µs. Sometime in the next few micro-
seconds after the switch cycle begins, the inductor current
will have risen to the 5A level of the load current and the
output voltage will stop dropping. At this point, the induc-
tor current will rise somewhat above the level of the output
current to replenish the charge lost from the output
capacitor during the load transient. During the next couple
of cycles, the MIN comparator may trip on and off,
preventing the output from falling below its –5% thresh-
old until the time constant of the compensation loop runs
out and the main feedback amplifier regains control. With
a properly compensated loop, the entire recovery time will
be inside of 10µs.
Most loads care only about the maximum deviation from
ideal, which occurs somewhere in the first two cycles after
the load step hits. During this time, the output capacitor
does all the work until the inductor and control loop regain
control. The initial drop (or rise if the load steps down) is
entirely controlled by the ESR of the capacitor and amounts
to most of the total voltage drop. To minimize this drop,
reduce the ESR as much as possible by choosing low ESR
capacitors and/or paralleling multiple capacitors at the
output. The capacitance value accounts for the rest of the
voltage drop until the inductor current rises. With most
output capacitors, several devices paralleled to get the
ESR down will have so much capacitance that this drop
term is negligible. Ceramic capacitors are an exception; a
small ceramic capacitor can have suitably low ESR with
relatively small values of capacitance, making this second
drop term significant.
Optimizing Loop Compensation
Loop compensation has a fundamental impact on tran-
sient recovery time, the time it takes the LTC1704 to
recover after the output voltage has dropped due to output
capacitor ESR. Optimizing loop compensation entails
maintaining the highest possible loop bandwidth while
ensuring loop stability. The Feedback Component Selec-
tion section describes in detail the techniques used to
design an optimized Type 3 feedback loop, appropriate for
most LTC1704 systems.
Measurement Techniques
Measuring transient response presents a challenge in two
respects: obtaining an accurate measurement and gener-
ating a suitable transient to use to test the circuit. Output
measurements should be taken with a scope probe di-
rectly across the output capacitor. Proper high frequency
probing techniques should be used. In particular, don’t
use the 6" ground lead that comes with the probe! Use an
adapter that fits on the tip of the probe and has a short
ground clip to ensure that inductance in the ground path
LTC1704/LTC1704B
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doesn’t cause a bigger spike than the transient signal
being measured. Conveniently, the typical probe tip ground
clip is spaced just right to span the leads of a typical output
capacitor. Make sure the bandwidth limit on the scope is
turned off, since a significant portion of the transient
energy occurs above the 20MHz cutoff.
Now that we know how to measure the signal, we need to
have something to measure. The ideal situation is to use
the actual load for the test, and switch it on and off while
watching the output. If this isn’t convenient, a current step
generator is needed. This generator needs to be able to
turn on and off in nanoseconds to simulate a typical
switching logic load, so stray inductance and long clip
leads between the LTC1704 and the transient generator
must be minimized.
Figure 12 shows an example of a simple transient genera-
tor. Be sure to use a noninductive resistor as the load
element—many power resistors use an inductive spiral
pattern and are not suitable for use here. A simple solution
is to take ten 1/4W film resistors and wire them in parallel
to get the desired value. This gives a noninductive resistive
load which can dissipate 2.5W continuously or 50W if
pulsed with a 5% duty cycle, enough for most LTC1704
circuits. Solder the MOSFET and the resistor(s) as close to
the output of the LTC1704 circuit as possible and set up
the signal generator to pulse at a 100Hz rate with a 5% duty
cycle. This pulses the LTC1704 with 500µs transients
10ms apart, adequate for viewing the entire transient
recovery time for both positive and negative transitions
while keeping the load resistor cool.
LINEAR REGULATOR SUPPLY
Linear Regulator Output Voltage
The linear regulator senses the output voltage at V
OUTREG
with an internal amplifier (see Figure 13). The amplifier
negative input is connected internally to an 800mV refer-
ence, while the positive input is connected to the REGFB
pin. The amplifier output drives a P-channel transistor
MREG, which is in turn connected to the external NPN pass
transistor. The linear regulator output voltage can be
obtained using the following equation:
VV
R
R
OUTREG
=+
08 1
5
6
.
Figure 12. Transient Load Generator
LTC1704
V
OUTSW
IRFZ44 OR
EQUIVALENT
R
LOAD
50
0V TO 10V
100Hz, 5%
DUTY CYCLE
LOCATE CLOSE TO THE OUTPUT
1704 F12
PULSE
GENERATOR
Figure 13. Linear Regulator
QEXT
MOFF
R5
R6
REGDR
REGILM
MREG
V
CC
V
REF
2mA
REGFB
1704 F13
+
C
OUTREG
V
OUTREG
V
REGON
R
REGILM
C
DELAY
I
P
V
INREG
REGOFF
V
CC
1.9µA
LTC1704
REG
ILM
+
REGFB
+
AMP
Linear Regulator Supplies Requirement
The linear regulator operates with two supplies: V
CC
for the
LTC1704 and V
INREG
for the external NPN transistor QEXT.
Both supplies must be higher than the minimum value
determined by the linear regulator output voltage, V
OUTREG
.
For a desired V
OUTREG
, use the following formula to
calculate the minimum required V
CC
:
Minimum V
CC
= V
OUTREG
+ V
BE(QEXT)
+ V
DROPOUT

LTC1704EGN#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Step-Down DC/DC Controller
Lifecycle:
New from this manufacturer.
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