LT3971A/LT3971A-5
13
3971af
maximum input voltage (V
IN(OP-MAX)
) that guarantees
optimum output voltage ripple for that application can be
found by applying the following equation:
V
IN(OP-MAX)
=
V
OUT
+ V
D
f
SW
•t
ON(MIN)
–V
D
+ V
SW
where t
ON(MIN)
is the minimum switch on-time. Note that
a higher switching frequency will decrease the maximum
operating input voltage. Conversely, a lower switching
frequency will be necessary to achieve normal operation
at higher input voltages.
The circuit will tolerate inputs above the maximum op-
erating input voltage and up to the Absolute Maximum
Ratings of the V
IN
and BOOST pins, regardless of chosen
switching frequency. However, during such transients
where V
IN
is higher than V
IN(OP-MAX)
, the LT3971A will
enter pulse-skipping operation where some switching
pulses are skipped to maintain output regulation. The
output voltage ripple and inductor current ripple will be
higher than in typical operation. Do not overload when
V
IN
is greater than V
IN(OP-MAX)
.
Inductor Selection and Maximum Output Current
A good first choice for the inductor value is:
L =
V
OUT
+ V
D
f
SW
where f
SW
is the switching frequency in MHz, V
OUT
is the
output voltage, V
D
is the catch diode drop (~0.5V) and L
is the inductor value in H.
The inductors 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 3.5A. To keep the
efficiency high, the series resistance (DCR) should be less
than 0.1, and the core material should be intended for
high frequency applications. Table 2 lists several vendors
and suitable types.
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 LT3971A limits its peak switch current in order to
protect itself and the system from overload faults. The
LT3971As switch current limit (I
LIM
) is typically 2.5A at low
duty cycles and decreases linearly to 1.75A at DC = 0.8.
Table 2. Inductor Vendors
VENDOR URL PART SERIES TYPE
Murata www.murata.com LQH55D Open
TDK www.componenttdk.com SLF7045
SLF10145
Shielded
Shielded
Toko www.toko.com D62CB
D63CB
D73C
D75F
Shielded
Shielded
Shielded
Open
Coilcraft www.coilcraft.com MSS7341
MSS1038
Shielded
Shielded
Sumida www.sumida.com CR54
CDRH74
CDRH6D38
CR75
Open
Shielded
Shielded
Open
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
=
(1DC) (V
OUT
+ V
D
)
L•f
SW
APPLICATIONS INFORMATION
LT3971A/LT3971A-5
14
3971af
Where f
SW
is the switching frequency of the LT3971A, DC is
the duty cycle and L is the value of the inductor. Therefore,
the maximum output current that the LT3971A 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 details of maximum output cur-
rent and discontinuous operation, see Linear Technologys
Application Note 44. Finally, for duty cycles greater than
50% (V
OUT
/V
IN
>0.5), a minimum inductance is required to
avoid sub-harmonic oscillations. See Application Note 19.
One approach to choosing the inductor is to start with
the simple rule given above, look at the available induc-
tors, and choose one to meet cost or space goals. Then
use the equations above to check that the LT3971A 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 I
L
/2.
Input Capacitor
Bypass the input of the LT3971A circuit with a ceramic
capacitor of X7R or X5R type. Y5V types have poor
performance over temperature and applied voltage, and
should not be used. A 4.7F to 10F ceramic capacitor
is adequate to bypass the LT3971A and will easily handle
the ripple current. 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 LT3971A and to force this very high frequency
switching current into a tight local loop, minimizing EMI.
A 4.7F capacitor is capable of this task, but only if it is
placed close to the LT3971A (see the PCB Layout sec-
tion). A second precaution regarding the ceramic input
capacitor concerns the maximum input voltage rating of
the LT3971A. A ceramic input capacitor combined with
trace or cable inductance forms a high quality (under
damped) tank circuit. If the LT3971A circuit is plugged
into a live supply, the input voltage can ring to twice its
nominal value, possibly exceeding the LT3971As voltage
rating. This situation is easily avoided (see the Hot Plug-
ging Safely section).
Output Capacitor and Output Ripple
The output capacitor has two essential functions. Along
with the inductor, it filters the square wave generated
by the LT3971A to produce the DC output. In this role it
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 LT3971As control loop. Ceramic capacitors
have very low equivalent series resistance (ESR) and pro-
vide the best ripple performance. A good starting value is:
C
OUT
=
100
V
OUT
f
SW
where f
SW
is in MHz, and C
OUT
is the recommended output
capacitance in F. Use X5R or X7R types. This choice will
provide low output ripple and good transient response.
Transient performance can be improved with a higher
value capacitor. Increasing the output capacitance will
also decrease the output voltage ripple. A lower value of
output capacitor can be used to save space and cost but
transient performance will suffer.
APPLICATIONS INFORMATION
LT3971A/LT3971A-5
15
3971af
APPLICATIONS INFORMATION
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 3 lists several capacitor vendors.
Table 3. Recommended Ceramic Capacitor Vendors
MANUFACTURER WEBSITE
AVX www.avxcorp.com
Murata www.murata.com
Taiyo Yuden www.t-yuden.com
Vishay Siliconix www.vishay.com
TDK www.tdk.com
Catch Diode Selection
The catch diode (D1 from Block Diagram) conducts cur-
rent only during switch off time. Average forward current
in normal operation can be calculated from:
I
D(AVG)
=I
OUT
V
IN
–V
OUT
V
IN
where I
OUT
is the output load current. The only reason to
consider a diode with a larger current rating than necessary
for nominal operation is for the worst-case condition of
shorted output. The diode current will then increase to the
typical peak switch current. Peak reverse voltage is equal
to the regulator input voltage. Use a diode with a reverse
voltage rating greater than the input voltage.
Table 4. Schottky Diodes. The Reverse Current Values Listed Are
Estimates Based Off of Typical Curves for Reverse Current
vs Reverse Voltage at 25°C.
PART NUMBER
V
R
(V)
I
AVE
(A)
V
F
at 1A
(mV)
V
F
at 2A
(mV)
I
R
at V
R
=
20V 25°C
(µA)
On Semiconductor
MBR0520L 20 0.5 30
MBR0540 40 0.5 620 0.4
MBRM120E 20 1 530 595 0.5
MBRM140 40 1 550 20
Diodes Inc.
B0530W 30 0.5 15
B0540W 40 0.5 620 1
B120 20 1 500 1.1
B130 30 1 500 1.1
B140 40 1 500 1.1
B150 50 1 700 0.4
B220 20 2 500 20
B230 30 2 500 0.6
B140HB 40 1 1
DFLS240L 40 2 500 4
DFLS140 40 1.1 510 1
DFLS160 60 1 500 2.5
DFLS2100 100 2 770 860 0.01
B240 40 2 500 0.45
Central Semiconductor
CMSH1 - 40M 40 1 500
CMSH1 - 60M 60 1 700
CMSH1 - 40ML 40 1 400
CMSH2 - 40M 40 2 550
CMSH2 - 60M 60 2 700
CMSH2 - 40L 40 2 400
CMSH2 - 40 40 2 500
CMSH2 - 60M 60 2 700

LT3971AIMSE-5#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 40V, 1.2A, 2MHz Step-Down Switching Regulator with 2uA Quiescent Current
Lifecycle:
New from this manufacturer.
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