10
LT1738
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The current slew feedback loop consists of the voltage
across the external sense resistor, which is internally
amplified and differentiated. The derivative is limited to a
value set by R
CSL
. The current slew rate is thus inversely
proportional to both the value of sense resistor and R
CSL.
The two control loops are combined internally so that a
smooth transition from current slew control to voltage
slew control is obtained. When turning on, the driver
current will slew before voltage. When turning off, voltage
will slew before current. In general it is desirable to have
R
VSL
and R
CSL
of similar value.
Internal Regulator
Most of the control circuitry operates from an internal 2.4V
low dropout regulator that is powered from V
IN
. The
internal low dropout design allows V
IN
to vary from 2.7V
to 20V with stable operation of the controller. When SHDN
< 1.3V the internal regulator is completely disabled.
5V Regulator
A 5V regulator is provided for powering external circuitry.
This regulator draws current from V
IN
and requires V
IN
to
be greater than 6.5V to be in regulation. It can sink or
source 10mA. The output is current limited to prevent
against destruction from accidental short circuits.
Safety and Protection Features
There are several safety and protection features on the
chip. The first is overcurrent limit. Normally the gate driver
will go low when the output of the internal sense amplifier
exceeds the voltage on the V
C
pin. The V
C
pin is clamped
such that maximum output current is attained when the CS
pin voltage is 0.1V. At that level the outputs will be
immediately turned off (no slew). The effect of this control
is that the output voltage will foldback with overcurrent.
In addition, if the CS voltage exceeds 0.22V, the V
C
and SS
pins will be discharged to ground, resetting the soft-start
function. Thus if a short is present this will allow for faster
MOSFET turnoff and less MOSFET stress.
If the voltage on the FB pin exceeds regulation by approxi-
mately 0.22V, the outputs will immediately go low. The
implication is that there is an overvoltage fault.
The voltage on GCL determines two features. The first is
the maximum gate drive voltage. This will protect the
MOSFET gate from overvoltage.
With GCL tied to a zener or an external voltage source then
the maximum gate driver voltage is approximately
V
GCL
– 0.2V. If GCL is tied to V
IN
, then the maximum gate
voltage is determined by V
IN
and is approximately
V
IN
– 1.6V. There is an internal 19V zener on the GCL pin
that prevents the gate driver pin from exceeding approxi-
mately 19V.
In addition, the GCL voltage determines undervoltage
lockout of the gate drive. This feature disables the gate
driver if V
IN
is too low to provide adequate voltage to turn
on the MOSFET. This is helpful during start up to insure the
MOSFET has sufficient gate drive to saturate.
If GCL is tied to a voltage source or zener less than 6.8V,
the gate driver will not turn on until V
IN
exceeds GCL
voltage by 0.8V. For V
GCL
above 6.5V, the gate drive is
insured to be off for V
IN
< 7.3V and it will be turned on by
V
GCL
+ 0.8V.
If GCL is tied to V
IN
, the gate driver is always on
(undervoltage lockout is disabled).
The gate drive has current limits for the drive currents. If
the sink or source current is greater than 300mA then the
current will be limited.
The V5 regulator also has internal current limiting that will
only guarantee ±10mA output current.
There is also an on chip thermal shutdown circuit that will
turn off the output in the event the chip temperature rises
to dangerous levels. Thermal shutdown has hysteresis
that will cause a low frequency (<1kHz) oscillation to occur
as the chip heats up and cools down.
The chip has an undervoltage lockout feature that will
force the gate driver low in the event that V
IN
drops below
2.5V. This insures predictable behavior during start up and
shut down. SHDN can be used in conjuction with an
external resistor divider to completely disable the part if
the input voltage is too low. This can be used to insure
adequate voltage to reliably run the converter. See the
section in Applications Information.
Table 1 summarizes these features.
OPERATIO
U
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LT1738
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APPLICATIO S I FOR ATIO
WUU
U
OPERATIO
U
Reducing EMI from switching power supplies has tradi-
tionally invoked fear in designers. Many switchers are
designed solely on efficiency and as such produce wave-
forms filled with high frequency harmonics that then
propagate through the rest of the system.
The LT1738 provides control over two of the more impor-
tant variables for controlling EMI with switching inductive
loads: switch voltage slew rate and switch current slew
rate. The use of this part will reduce noise and EMI over
conventional switch mode controllers. Because these
variables are under control, a supply built with this part will
exhibit far less tendency to create EMI and less chance of
encountering problems during production.
It is beyond the scope of this data sheet to get into EMI
fundamentals. Application Note 70 contains much infor-
mation concerning noise in switching regulators and
should be consulted.
Oscillator Frequency
The oscillator determines the switching frequency and
therefore the fundamental positioning of all harmonics.
The use of good quality external components is important
to ensure oscillator frequency stability. The oscillator is of
a sawtooth design. A current defined by external resistor
R
T
is used to charge and discharge the capacitor C
T
. The
discharge rate is approximately ten times the charge rate.
By allowing the user to have control over both compo-
nents, trimming of oscillator frequency can be more easily
achieved.
The external capacitance C
T
is chosen by:
CnF
f kHz R k
T
T
()
()()
=
2180
where f is the desired oscillator frequency in kHz. For R
T
equal to 16.9k, this simplifies to:
CnF
f kHz
T
()
()
=
129
e.g., C
T
= 1.29nF for f = 100kHz
Nominally R
T
should be 16.9k. Since it sets up current, its
temperature coefficient should be selected to compliment
the capacitor. Ideally, both should have low temperature
coefficients.
Table 1. Safety and Protection Features
FEATURE FUNCTION EFFECT on GATE DRIVER SLEW CONTROL EFFECT on V
C
, SS
Maximum Current Fault Turn Off FET at Maximum Immediately Goes Low Overridden None
Switch Current (V
SENSE
= 0.1)
Short-Circuit Fault Turn Off FET and Reset V
C
Immediately Goes Low Overridden Discharge V
C
, SS
for Short-Circuit (V
SENSE
= 0.22) to GND
Overvoltage Fault Turn Off Driver If FB > V
REG
+ 0.22V Immediately Goes Low Overridden None
(Output Overvoltage)
GCL Clamp Set Max Gate Voltage to Prevent Limits Max Voltage None None
FET Gate Breakdown
Gate Drive Disable Gate Drive When V
IN
Immediately Goes Low Overridden None
Undervoltage Lockout Is Too Low. Set Via GCL Pin
Thermal Shutdown Turn Off Driver If Chip Immediately Goes Low Overridden None
Temperature Is Too Hot
V
IN
Undervoltage Lockout Disable Part When V
IN
2.55V Immediately Goes Low Overridden None
Gate Drive Source and Sink Current Limit Limit Gate Drive Current Limit Drive Current None None
V5 Source/Sink Current Limit Limit Current from V5 None None None
Shutdown Disable Part When SHDN <1.3V
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APPLICATIO S I FOR ATIO
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U
Oscillator frequency is important for noise reduction in
two ways. First the lower the oscillator frequency the lower
the waveform’s harmonics, making it easier to filter them.
Second the oscillator will control the placement of the
output voltage harmonics which can aid in specific prob-
lems where you might be trying to avoid a certain fre-
quency bandwidth.
Oscillator Sync
If a more precise frequency is desired (e.g., to accurately
place harmonics) the oscillator can be synchronized to an
external clock. Set the RC timing components for an
oscillator frequency 10% lower than the desired sync
frequency.
Drive the SYNC pin with a square wave (with greater than
2V amplitude). The rising edge of the sync square wave
will initiate clock discharge. The sync pulse should have a
minimum pulse width of 0.5µs.
Be careful in sync’ing to frequencies much different from
the part since the internal oscillator charge slope deter-
mines slope compensation. It would be possible to get into
subharmonic oscillation if the sync doesn’t allow for the
charge cycle of the capacitor to initiate slope compensa-
tion. In general, this will not be a problem until the sync
frequency is greater than 1.5 times the oscillator free-run
frequency.
Slew Rate Setting
The primary reason to use this part is to gain advantage of
lower EMI and noise due to the slew control. The rolloff in
higher frequency harmonics has its theoretical basis with
two primary components. First, the clock frequency sets
the fundamental positioning of harmonics and second, the
associated normal frequency rolloff of harmonics.
This part creates a second higher frequency rolloff of
harmonics that inversely depends on the slew time, the
time that voltage or current spends between the off state
and on state. This time is adjustable through the choice of
the slew resistors, the external resistors to ground on the
R
VSL
and R
CSL
pins and the external components used for
the external voltage feedback capacitor C
V
(from CAP to
the MOSFET drain) and the sense resistor. Lower slew
rates (longer slew times, lower rolloff frequency for har-
monics ) are created with higher values of R
VSL
, R
CSL
, C
V
and the current sense resistor.
Setting the voltage and current slew rates should be done
empirically. The most practical way of determining these
components is to set C
V
and the sense resistor value.
Then, start by making R
VSL
, R
CSL
each a 50k resistor pot
in series with 3.3k. Starting from the lowest resistor
setting (fast slew) adjust the pots until the noise level
meets your guidelines. Note that slower slewing wave-
forms will dissipate more power so that efficiency will
drop. You can monitor this as you make your slew adjust-
ment by measuring input and output voltage and their
respective currents. Monitor the MOSFET temperature as
slew rates are slowed. The MOSFET will heat up as
efficiency decreases.
Measuring noise should be done carefully. It is easy to
introduce noise by poor measurement techniques. Con-
sult AN70 for recommended measurement techniques.
Keeping probe ground leads very short is essential.
Usually it will be desirable to keep the voltage and current
slew resistors approximately the same. There are circum-
stances where a better optimization can be found by
adjusting each separately, but as these values are sepa-
rated further, a loss of independence of control may occur.
It is possible to use a single slew setting resistor. In this
case the R
VSL
and R
CSL
pins are tied together. A resistor
with a value of 1.8k to 34k (one half the individual resis-
tors) can then be tied from these pins to ground.
In general only the R
CSL
value will be available for adjust-
ment of current slew. The current slew time also depends
on the current sense resistor but this resistor is normally
set with consideration of the maximum current in the
MOSFET.
Setting the voltage slew also involves selection of the
capacitor C
V
. The voltage slew time is proportional to the
output voltage swing (basically input voltage), the external
voltage feedback capacitor and the R
VSL
value. Thus at
higher input voltages smaller capacitors will be used with
lower R
VSL
values. For a starting point use Table␣ 2.

LT1738EG#PBF

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Analog Devices / Linear Technology
Description:
Switching Voltage Regulators SR Controlled Ultralow N DC/DC Cntr
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