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LT3697
22
3697f
applicaTions inForMaTion
Inductor Selection and Maximum Output Current
For a given input and output voltage, the inductor value
and switching frequency will determine the ripple current.
The ripple current increases with higher V
IN
or V
OUT
and
decreases with higher inductance and faster switching
frequency. A good first choice for the inductor value is:
L =
V
SYS
+ V
D
1.5 f
SW
where f
SW
is the switching frequency in MHz, V
SYS
is the
SYS pin voltage, V
D
is the catch diode drop (~0.5V) and
L is the inductor value is μH.
The inductor’s RMS current rating must be greater than the
maximum load current and its saturation current should be
about 30% higher. For robust operation in fault conditions
(start-up or short circuit) and high input voltage (>30V), the
saturation current should be above 7A. To keep the efficiency
high, the series resistance (DCR) should be less than 0.1Ω,
and the core material should be intended for high frequency
applications. Table 4 lists several inductor vendors.
Table 4. Inductor Vendors
VENDOR URL
Coilcraft www.coilcraft.com
Sumida www.sumida.com
Toko www.tokoam.com
Würth Electronik www.we-online.com
Coiltronics www.cooperet.com
Murata www.murata.com
The inductor value must be sufficient to supply the desired
maximum output current (I
OUT(MAX)
), which is a function
of the switch current limit (I
LIM
) and the ripple current.
I
OUT(MAX)
= I
LIM
ΔI
L
2
The LT3697 limits its peak switch current in order to protect
itself and the system from overload faults. The LT3697’s
switch current limit (I
LIM
) is 5.3A at low duty cycles and
decreases linearly to 4A at DC = 0.8.
When the switch is off, the potential across the inductor
is the output voltage plus the catch diode drop. This gives
the peak-to-peak ripple current in the inductor:
ΔI
L
=
(1–DC)(V
SYS
+
V
D
)
L f
SW
where f
SW
is the switching frequency of the LT3697, DC is
the duty cycle and L is the value of the inductor. Therefore,
the maximum output current that the LT3697 will deliver
depends on the switch current limit, the inductor value,
and the input and output voltages. The inductor value may
have to be increased if the inductor ripple current does
not allow sufficient maximum output current (I
OUT(MAX)
)
given the switching frequency and maximum input voltage
used in the desired application.
The optimum inductor for a given application may differ
from the one indicated by this simple design guide. A larger
value inductor provides a higher maximum load current
and reduces the output voltage ripple. If your load is lower
than the maximum load current, than you can relax the
value of the inductor and operate with higher ripple cur
-
rent. This allows you to use a physically smaller inductor,
or one with a lower DCR resulting in higher efficiency. Be
aware that if the inductance differs from the simple rule
above, then the maximum load current will depend on
the input voltage. In addition, low inductance may result
in discontinuous mode operation, which further reduces
maximum
load current. For discussion regarding maximum
output current and discontinuous operation, see Linear
Technology’s Application Note 44. Additionally, for duty
cycles greater than 50% (V
OUT
/V
IN
> 0.5), a minimum
inductance is required to avoid subharmonic oscillations,
see Application Note 19.
Figure 8. V
IN
to V
OUT
Performance
R
LOAD
= 100Ω
(50mA IN REGULATION)
R
CBL
= ∞
100ms/DIV
2V/DIV
3697 F08
V
IN
V
OUT
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LT3697
23
3697f
applicaTions inForMaTion
One approach to choosing the inductor is to start with the
simple rule given above, look at the available inductors,
and choose one to meet cost or space goals. Then use the
equations above to check that the LT3697 will be able to
deliver the required output current. Note again that these
equations assume that the inductor current is continuous.
Discontinuous operation occurs when I
OUT
is less than:
ΔI
L
2
Input Capacitor
Bypass the
input of the LT3697 circuit with a ceramic capaci-
tor of
X7R or X5R type. Y5V types have poor performance
over
temperature and applied voltage, and should not be
used. A 4.7μF to 10μF ceramic capacitor is adequate to
bypass the LT3697 and will easily handle the ripple cur
-
rent. Note that larger input capacitance is required when
a
lower switching frequency is used (due to longer on
times). If the input power source has high impedance, or
there is significant inductance due to long wires or cables,
additional bulk capacitance may be necessary. This can
be provided with a low performance electrolytic capacitor.
Step-down regulators draw current from the input sup
-
ply in pulses with very fast rise and fall times. The input
capacitor
is required to reduce the resulting voltage ripple
at the LT3697 input and to force this very high frequency
switching current into a tight local loop, minimizing EMI.
A 4.7μF capacitor is capable of this task, but only if it is
placed close to the LT3697 (see the PCB Layout section).
A second precaution regarding the ceramic input capacitor
concerns the maximum input voltage rating
of the LT3697.
A
ceramic input capacitor combined with trace or cable
inductance forms a high quality (under damped) tank
circuit. If the LT3697 circuit is plugged into a live supply,
the input voltage can ring to twice its nominal value, pos
-
sibly exceeding
the LT3697’s voltage rating. If the input
supply is poorly controlled or the user will be plugging
the LT3697 into an energized supply, the input network
should be designed to prevent this overshoot. See Linear
Technology Application Note 88 for a complete discussion.
Output Capacitor and Output Ripple
The LT3697 output capacitors include C
OUT
tied to the
inductor and to the ISP side of R
SENSE
and C
BUS
tied to
the regulator output and the ISN side of R
SENSE
. These
output capacitors have two essential functions. Along
with the inductor, they filter the square wave generated by
the LT3697 to produce the DC output. In particular, C
OUT
determines the output ripple, so low impedance (at the
switching frequency) is important. The second function
is to store energy in order to satisfy transient loads and
stabilize the LT3697’s control loop.
C
BUS
serves some additional purposes. It helps to stabilize
the output current limit loop. To
this end, C
BUS
must satisfy
the following relationship:
C
BUS
≥ C
OUT
C
BUS
also helps provide the minimum 120µF bypassing
required for the VBUS rail as specified by the USB 2.0
standard document.
Ceramic capacitors have very low equivalent series re
-
sistance (ESR) and
provide the best ripple performance.
A good starting value for C
OUT
is 47µF in 1206 or 1210
case size. Use X5R or X7R types. A good starting value
for C
BUS
is 100µF. Since C
BUS
is only tied to the inductor
through RSENSE, the ESR rating of C
BUS
is less critical
and high density tantalum or electrolytic capacitor types
may be used.
When choosing a capacitor, look carefully through the
data sheet to find out what the actual capacitance is under
operating conditions (applied voltage and temperature).
A physically larger capacitor or one with a higher voltage
rating may be required. Table 5 lists several capacitor
vendors.
Table 5. Recommended Ceramic Capacitor Vendors
MANUFACTURER URL
AVX www.avxcorp.com
Murata www.murata.com
Taiyo Yuden www.t-yuden.com
Vishay Siliconix www.vishay.com
TDK www.tdk.com
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LT3697
24
3697f
applicaTions inForMaTion
Catch Diode Selection
The catch diode (D
CATCH
from the Block Diagram) conducts
current only during the switch off time. Average forward
current in normal operation can be calculated from:
I
D(AVG)
= I
OUT
V
IN
V
SYS
( )
V
IN
where I
OUT
is the output load current. The current rating of
the diode should be selected to be greater than or equal to
the application’s output load current, so that the diode is
robust for a wide input voltage range. The voltage rating of
the diode is equal to the maximum regulator input voltage
while switching, 37V or less. Use a 3A, 40V Schottky diode.
Do not use a 60V diode due to the high resistive voltage drop.
BST and SYS Pin Considerations
Capacitor C
BST
and Schottky diode D
BST
(see the Block
Diagram) are used to generate a boost voltage that is
higher than the input voltage to drive the internal NPN
power switch. In most cases a 0.47μF capacitor will work
well for C
BST
. For switching frequency below 500kHz, use
1µF. The BST pin must be more than 1.8V above the SW
pin for best efficiency and more than 2.6V above the SW
pin to allow the LT3697 to skip off times to achieve very
high duty cycles.
With the SYS pin connected to the output, a 180mA ac
-
tive load will charge the boost capacitor during light load
start-up and an enforced 600mV minimum dropout voltage
will
keep the boost capacitor charged across operating
conditions (see Minimum Dropout Voltage section).
Enable
The LT3697 is in shutdown with I
VIN
< 1µA when the EN
pin is low and active when the pin is high. The enable
threshold is about 1.5V. The EN pin can be tied to V
IN
if the shutdown feature is not used. The EN pin current
depends on the EN pin voltage for V
EN
< 12V and reaches
about 30µA at 12V.
Synchronization
To select low ripple Burst Mode operation, tie the SYNC
pin below 0.3V (this can be ground or a logic output).
Synchronizing the LT3697 oscillator to an external fre
-
quency can be done by connecting a square wave (with
on
and off time greater than 50ns) to the SYNC pin. The
square wave amplitude should have valleys that are below
0.4V and peaks above 1V (up to 6V).
The LT3697 will skip pulses at low output loads while
synchronized to an external clock to maintain regula
-
tion. At very light loads, the part will go to sleep between
groups of pulses, reducing the quiescent current of the
part. Holding the SYNC pin DC high yields no advantages
so
it is not recommended.
The LT3697 may be synchronized over a 300kHz to
2.2MHz range. The R
T
resistor should be chosen to set
the LT3697 switching frequency 10% below the lowest
synchronization input. For example, if the synchroniza
-
tion signal will be 300kHz and higher, the R
T
should be
selected for 270kHz. To ensure reliable and safe operation
the LT3697 will only synchronize when the output voltage
is near regulation. It is therefore necessary to choose a
large enough inductor value to supply the required output
current at the frequency set by the R
T
resistor (see Induc-
tor Selection section). The slope compensation is set by
the
R
T
value, while the minimum slope compensation
required to avoid subharmonic oscillations is established
by the inductor size, input voltage and output voltage.
Since the synchronization frequency will not change the
slopes of the inductor current waveform, if the inductor
is large enough to avoid subharmonic oscillations at the
frequency set by R
T
, than the slope compensation will be
sufficient for all synchronization frequencies.
Shorted and Reversed Input Protection
If the inductor is chosen so that it won’t saturate excessively,
the LT3697 will tolerate a shorted output and the
power
dissipation
will be limited by the current limit set by R
LIM
and R
SENSE
(see the Setting the Current Limit section).
There is another situation to consider in systems where
the output will be held high when the input to the LT3697
is absent. This may occur in automotive systems where
the LT3697 output may be connected to the 12V V
BATT
during a fault condition or if a USB peripheral with a
large, charged cap is plugged into the LT3697 output. If
the V
IN
pin is allowed to float and the EN pin is held high

LT3697IMSE#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators USB 5V, 2.5A, 40V Input Step-Down Switching Regulator with Cable Drop Compensation
Lifecycle:
New from this manufacturer.
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