10
LT3431
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APPLICATIO S I FOR ATIO
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importance, the subsequent suggestions in Peak Induc-
tor and Fault Current and EMI will additionally help in the
selection of the inductor value.
Peak-to-peak output ripple voltage is the sum of a triwave
(created by peak-to-peak ripple current (I
LP-P
) times ESR)
and a square wave (created by parasitic inductance (ESL)
and ripple current slew rate). Capacitive reactance is
assumed to be small compared to ESR or ESL.
V I ESR ESL
dI
dt
RIPPLE LP P
=
()()
+
()
-
Σ
where:
ESR = equivalent series resistance of the output
capacitor
ESL = equivalent series inductance of the output
capacitor
dI/dt = slew rate of inductor ripple current = V
IN
/L
Peak-to-peak ripple current (I
LP-P
) through the inductor
and into the output capacitor is typically chosen to be
between 20% and 40% of the maximum load current. It is
approximated by:
I
VVV
VfL
LP P
OUT IN OUT
IN
-
=
()( )
()()()
Example: with V
IN
= 12V, V
OUT
= 5V, L = 10µH, ESR =
0.080 and ESL = 10nH, output ripple voltage can be
approximated as follows:
IA
dI
dt
VA
mV
RIPPLE
P-P
P-P
=
()
()
()
()()
=
==
=
()()
+
()()
()
=+=
512 5
12 10 10 500 10
058
12
10 10
10 1 2
0 58 0 08 10 10 10 1 2
0 046 0 012 58
63
6
6
96
••
.
•.
.. .
..
Σ
To reduce output ripple voltage further requires an in-
crease in the inductor value with the trade-off being a
physically larger inductor with the possibility of increased
component height and cost.
Ceramic Output Capacitor
An alternative way to further reduce output ripple voltage
is to reduce the ESR of the output capacitor by using a
ceramic capacitor. Although this reduction of ESR re-
moves a useful zero in the overall loop response, this zero
can be replaced by inserting a resistor (R
C
) in series with
the V
C
pin and the compensation capacitor C
C
. (See
Ceramic Capacitors in Applications Information.)
Peak Inductor Current and Fault Current
To ensure that the inductor will not saturate, the peak
inductor current should be calculated knowing the maxi-
mum load current. An appropriate inductor should then
be chosen. In addition, a decision should be made whether
or not the inductor must withstand continuous fault
conditions.
If maximum load current is 1A, for instance, a 1A inductor
may not survive a continuous 4A overload condition. Dead
shorts will actually be more gentle on the inductor because
the LT3431 has frequency and current limit foldback.
Peak inductor and switch current can be significantly
higher than output current, especially with smaller induc-
tors and lighter loads, so don’t omit this step. Powdered
iron cores are forgiving because they saturate softly,
whereas ferrite cores saturate abruptly. Other core mate-
rials fall somewhere in between. The following formula
assumes continuous mode of operation, but errs only
slightly on the high side for discontinuous mode, so it can
be used for all conditions.
II
I
I
VVV
VfL
PEAK OUT
LP P
OUT
OUT IN OUT
IN
=+ =+
()( )
()( )()()
()
-
2
2
EMI
Decide if the design can tolerate an “open” core geometry
like a rod or barrel, which have high magnetic field
radiation, or whether it needs a closed core like a toroid to
prevent EMI problems. This is a tough decision because
the rods or barrels are temptingly cheap and small and
11
LT3431
sn3431 3431fs
APPLICATIO S I FOR ATIO
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Additional Considerations
After making an initial choice, consider additional factors
such as core losses and second sourcing, etc. Use the
experts in Linear Technology’s Applications department if
you feel uncertain about the final choice. They have
experience with a wide range of inductor types and can tell
you about the latest developments in low profile, surface
mounting, etc.
Maximum Output Load Current
Maximum load current for a buck converter is limited by
the maximum switch current rating (I
P
). The current rating
for the LT3431 is 3A. Unlike most current mode convert-
ers, the LT3431 maximum switch current limit does not
fall off at high duty cycles. Most current mode converters
suffer a drop off of peak switch current for duty cycles
above 50%. This is due to the effects of slope compensa-
tion required to prevent subharmonic oscillations in cur-
rent mode converters. (For detailed analysis, see Applica-
tion Note 19.)
The LT3431 is able to maintain peak switch current limit
over the full duty cycle range by using patented circuitry to
cancel the effects of slope compensation on peak switch
current without affecting the frequency compensation it
provides.
Maximum load current would be equal to maximum
switch current
for an infinitely large inductor
, but with
finite inductor size, maximum load current is reduced by
one-half peak-to-peak inductor current (I
LP-P
). The follow-
ing formula assumes continuous mode operation, imply-
ing that the term on the right is less than one-half of I
P
.
I
OUT(MAX)
=
Continuous Mode
I–
I
2
=I
P
LP-P
P
+
()
()
()()( )
VVVVV
LfV
OUT F IN OUT F
IN
2
For V
OUT
= 5V, V
IN
= 12V, V
F(D1)
= 0.52V, f = 500kHz
and L = 10µH:
I
A
OUT MAX
()
=−
+
()
()
()()
()
=− =
3
5 0 52 12 5 0 52
2 15 10 500 10 12
30327
63
.–.
••
..
Note that there is less load current available at the higher
input voltage because inductor ripple current increases. At
V
IN
= 24V, duty cycle is 23% and for the same set of
conditions:
I
A
OUT MAX()
.–.
••
..
=−
+
()
()
()()
()
=− =
3
5 0 52 24 5 0 52
2 15 10 500 10 24
3 0 43 2 57
63
Table 2
VENDOR/ VALUE I
DC
DCR HEIGHT
PART NUMBER (
µ
H) (Amps) (Ohms) (mm)MAX
Sumida
CDRH8D28-4R7 4.7 3.4 0.019 3
CDRH8D28-7R3 7.3 2.8 0.030 3
CDRH8D43-100 10 4 0.029 4.5
CDRH8D43-150 15 2.9 0.042 4.5
CEI122-100 10 3.4 0.029 3
CEI122(H)-150 15 3.6 0.071 3
CDRH104R-150 15 3.6 0.037 4
CDRH104R-220 22 2.9 0.054 4
CDRH124-330 33 2.9 0.066 4.5
Coiltronics
UP2B-6R8 6.8 3.6 0.020 6
UP2B-100 10 3.3 0.027 6
UP3B-220 22 3.7 0.049 6.8
UP3B-330 33 3.0 0.069 6.8
Coilcraft
DO1813P-472 4.7 2.6 0.054 5
DS3316P-472 4.7 3.2 0.054 5.08
DS3316P-682 6.8 2.8 0.075 5.08
DO3316P-103 10 3.8 0.038 5.21
DO3316P-153 15 3.0 0.046 5.21
there are no helpful guidelines to calculate when the
magnetic field radiation will be a problem.
12
LT3431
sn3431 3431fs
APPLICATIO S I FOR ATIO
WUUU
To calculate actual peak switch current with a given set of
conditions, use:
II
I
VVVVV
LfV
SW PEAK
OUT
P
OUT
OUT F IN OUT F
IN
()
=+
=+
+−
()
()()( )
I
2
L-P
()
2
Reduced Inductor Value and Discontinuous Mode
If the smallest inductor value is of most importance to a
converter design, in order to reduce inductor size/cost,
discontinuous mode may yield the smallest inductor solu-
tion. The maximum output load current in discontinuous
mode, however, must be calculated and is defined later in
this section.
Discontinuous mode is entered when the output load
current is less than one-half of the inductor ripple
current (I
LP-P
). In this mode, inductor current falls to
zero before the next switch turn on (see Figure 8). Buck
converters will be in discontinuous mode for output
load current given by:
I
OUT
Discontinuous Mode
The inductor value in a buck converter is usually chosen
large enough to keep inductor ripple current (I
LP-P
) low;
this is done to minimize output ripple voltage and maxi-
mize output load current. In the case of large inductor
values, as seen in the equation above, discontinuous
mode will be associated with “light loads.”
When choosing small inductor values, however, discon-
tinuous mode will occur at much higher output load
currents. The limit to the smallest inductor value that can
be chosen is set by the LT3431 peak switch current (I
P
)
and the maximum output load current required, given by:
Example: For V
IN
= 12V, V
OUT
= 5V, V
F
= 0.52V, f = 500kHz
and L = 2.2µH.
I
OUT(MAX)
Discontinuous
Mode
I
OUT(MAX)
= 1.66A
Discontinuous Mode
What has been shown here is that if high inductor ripple
current and discontinuous mode operation can be toler-
ated, small inductor values can be used. If a higher output
load current is required, the inductor value must be
increased. If I
OUT(MAX)
no longer meets the discontinuous
mode criteria, use the I
OUT(MAX)
equation for continuous
mode; the LT3431 is designed to operate well in both
modes of operation, allowing a large range of inductor
values to be used.
Short-Circuit Considerations
For a ground short-circuit fault on the regulated output,
the maximum input voltage for the LT3431 is typically
limited to 21V. If a greater input voltage is required,
increasing the resistance in series with the inductor may
suffice (see short-circuit calculations at the end of this
section). Alternatively, the LT3430 can be used since it is
identical to the LT3431 but runs at a lower frequency of
200kHz, allowing higher sustained input voltage capability
during output short-circuit.
The LT3431 is a current mode controller. It uses the V
C
node voltage as an input to a current comparator which
turns off the output switch on a cycle-by-cycle basis as
peak current is reached. The internal clamp on the V
C
node, nominally 2V, then acts as an output switch peak
current limit. This action becomes the switch current limit
specification. The maximum available output power is
then determined by the switch current limit.
A potential controllability problem could occur under
short-circuit conditions. If the power supply output is
short circuited, the feedback amplifier responds to the low
output voltage by raising the control voltage, V
C
, to its
peak current limit value. Ideally, the output switch would
be turned on, and then turned off as its current exceeded
the value indicated by V
C
. However, there is finite response
<
+()()
()( )()()
VVVVV
VfL
OUT F IN OUT F
IN
2
=
=
()
+
I
IfLV
VVVVV
P
PIN
OUT F IN OUT F
2
2
2
2
()( )
••
()()
I
LP-P
=
+
3 500 10 4 7 10 12
25052125052
236
(•)(. )()
(.)(.)
I
OUT(MAX)
Discontinuous Mode

LT3431IFE#TRPBF

Mfr. #:
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Description:
Switching Voltage Regulators Hi V, 3A, 500kHz Buck Sw Reg
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