LT3435
13
3435fa
To calculate actual peak switch current in continuous
mode with a given set of conditions, use:
II
VVV
LfV
SW PK OUT
OUT IN OUT
IN
()
=+
()
()()( )
2
If a small inductor is chosen which results in discontinous
mode operation over the entire load range, the maximum
load current is equal to:
I
IfLV
VVV
OUT MAX
PK IN
OUT IN OUT
()
=
()( )( )
()( )
2
2
2
CHOOSING THE INDUCTOR
For most applications the output inductor will fall in the
range of 5µH to 33µH. Lower values are chosen to reduce
physical size of the inductor. Higher values allow more
output current because they reduce peak current seen by
the LT3435 switch, which has a 3A limit. Higher values
also reduce output ripple voltage and reduce core loss.
When choosing an inductor you might have to consider
maximum load current, core and copper losses, allow-
able component height, output voltage ripple, EMI, fault
current in the inductor, saturation and of course cost.
The following procedure is suggested as a way of han-
dling these somewhat complicated and conflicting
requirements.
1. Choose a value in microhenries such that
the maximum
load current plus half of the inductor ripple current is
less than the minimum peak switch current (I
PK
).
Choosing a small inductor with lighter loads may result
in discontinuous mode of operation, but the LT3435 is
designed to work well in either mode.
Assume that the average inductor current is equal to
load current and decide whether or not the inductor
must withstand continuous fault conditions. If maxi-
mum load current is 1A, for instance, a 1A inductor may
not survive a continuous 4A overload condition.
For applications with a duty cycle above 50%, the
inductor value should be chosen to obtain an inductor
ripple current of less than 40% of the peak switch
current.
2. Calculate peak inductor current at full load current to
ensure that the inductor will not saturate. Peak current
can be significantly higher than output current, especially
with smaller inductors 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 materials fall somewhere in between. The
following formula assumes continuous mode of opera-
tion, but it errs only slightly on the high side for discon-
tinuous mode, so it can be used for all conditions.
II
VVV
fLV
PEAK OUT
OUT IN OUT
IN
=+
()
()( )( )
2
V
IN
= maximum input voltage
f = switching frequency, 500kHz
Table 3. Inductor Selection Criteria
VENDOR/ VALUE I
DC(MAX)
DCR HEIGHT
PART NO. (
µ
H) (Amps) (Ohms) (mm)
Sumida
CDRH104R-4R7 4.7 6 0.013 4
CDRH104R-100 10 4.4 0.035 4
CDRH104R-150 15 3.6 0.050 4
CDRH104R-220 22 2.9 0.073 4
CDRH104R-330 33 2.3 0.093 4
CDRH124-4R7 4.7 5.7 0.015 4.5
CDRH124-100 10 4.5 0.026 4.5
CDRH124-220 22 2.9 0.066 4.5
CDRH124R-330 33 2.7 0.097 4.5
CDRH127-330 33 3.0 0.065 8
CEI122-220 22 2.3 0.085 34
Coiltronics
UP3B-4R7 4.7 6.5 0.0083 6.8
UP3B-4R7 10 4.3 0.026 6.8
UP3B-330 33 3 0.069 6.8
APPLICATIO S I FOR ATIO
WUUU
LT3435
14
3435fa
3. Decide if the design can tolerate an “open” core geom-
etry 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 there are no helpful guidelines to calculate
when the magnetic field radiation will be a problem.
4. After making an initial choice, consider the secondary
things like output voltage ripple, second sourcing, etc.
Use the experts in the 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.
Short-Circuit Considerations
The LT3435 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
this peak current is reached. The internal clamp on the V
C
node, nominally 2.2V, 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
time involved in both the current comparator and turn-off
of the output switch. These result in a minimum on time
t
ON(MIN).
When combined with the large ratio of V
IN
to
(V
F
+ I • R), the diode forward voltage plus inductor I • R
voltage drop, the potential exists for a loss of control.
Expressed mathematically the requirement to maintain
control is:
ft
VIR
V
ON
F
IN
+
where:
f = switching frequency
t
ON
= switch on time
V
F
= diode forward voltage
V
IN
= Input voltage
I • R = inductor I • R voltage drop
If this condition is not observed, the current will not be
limited at I
PK
but will cycle-by-cycle ratchet up to some
higher value. Using the nominal LT3435 clock frequency
of 500kHz, a V
IN
of 12V and a (V
F
+ I • R) of say 0.7V, the
maximum t
ON
to maintain control would be approximately
116ns, an unacceptably short time.
The solution to this dilemma is to slow down the oscillator
to allow the current in the inductor to drop to a sufficiently
low value such that the current doesn’t continue to ratchet
higher. When the FB pin voltage is abnormally low thereby
indicating some sort of short-circuit condition, the oscil-
lator frequency will be reduced. Oscillator frequency is
reduced by a factor of 4 when the FB pin voltage is below
0.4V and increases linearly to its typical value of 500kHz at
a FB voltage of 0.95V (see Typical Performance Character-
istics). In addition, if the current in the switch exceeds 1.5
• I
PK
current demanded by the V
C
pin, the LT3435 will skip
the next on cycle effectively reducing the oscillator fre-
quency by a factor of 2. These oscillator frequency reduc-
tions during short-circuit conditions allow the LT3435 to
maintain current control.
SOFT-START
For applications where [V
IN
/(V
OUT
+ V
F
)] ratios > 10 or
large input surge currents can’t be tolerated, the LT3435
soft-start feature should be used to control the output
capacitor charge rate during start-up, or during recovery
from an output short circuit thereby adding additional
control over peak inductor current. The soft-start function
limits the switch current via the V
C
pin to maintain a
constant voltage ramp rate (dV/dt) at the output capacitor.
A capacitor (C1 in Figure 2) from the C
SS
pin to the
regulated output voltage determines the output voltage
APPLICATIO S I FOR ATIO
WUUU
LT3435
15
3435fa
The minimum average input current depends on the V
IN
to
V
OUT
ratio, V
C
frequency compensation, feedback divider
network and Schottky diode leakage. It can be approxi-
mated by the following equation:
III
V
V
III
IN AVG VINS SHDN
OUT
IN
BIASS FB S
()
++
++
()
()
η
where
I
VINS
= input pin current in sleep mode
V
OUT
= output voltage
V
IN
=
input voltage
I
BIASS
= BIAS pin current in sleep mode
I
FB
= feedback network current
I
S
= catch diode reverse leakage at V
OUT
η = low current efficiency (non Burst Mode operation)
Example: For V
OUT
= 3.3V, V
IN
= 12V
IAA
AAA
AA A A
IN AVG()
.( . . )
(.)
+µ+
µ+ µ+ µ
+µ+µ
45 5
33
12
125 12 5 0 5
08
45 5 44 99
Burst Mode OPERATION
To enhance efficiency at light loads, the LT3435 automati-
cally switches to Burst Mode operation which keeps the
output capacitor charged to the proper voltage while
minimizing the input quiescent current. During Burst
Mode operation, the LT3435 delivers short bursts of
current to the output capacitor followed by sleep periods
where the output power is delivered to the load by the
output capacitor. In addition, V
IN
and BIAS quiescent
currents are reduced to typically 45µA and 125µA respec-
tively during the sleep time. As the load current decreases
towards a no load condition, the percentage of time that
the LT3435 operates in sleep mode increases and the
average input current is greatly reduced resulting in higher
efficiency.
Figure 4. V
OUT
dV/dt
Figure 5. I
Q
vs V
IN
V
OUT
1V/DIV
V
IN
= 12V 1ms/DIV 3435 F04
V
OUT
= 3.3V
I
L
= 500mA
ramp rate. When the current through the C
SS
capacitor
exceeds the C
SS
threshold (I
CSS
), the voltage ramp of the
output capacitor is limited by reducing the V
C
pin voltage.
The C
SS
threshold is proportional to the FB voltage (see
Typical Performance Characteristics) and is defeated for
FB voltages greater than 0.9V (typical). The output dV/dt
can be approximated by:
dV
dt
I
C
CSS
SS
=
but actual values will vary due to start-up load conditions,
compensation values and output capacitor selection.
APPLICATIO S I FOR ATIO
WUUU
INPUT VOLTAGE (V)
0
0
SUPPLY CURRENT (µA)
50
100
10
20
30 40
3435 F05
50
150
25
75
125
60
V
OUT
= 3.3V
T
A
= 25°C
During the sleep portion of the Burst Mode Cycle, the V
C
pin voltage is held just below the level need for normal
operation to improve transient response. See the Typical
Performance Characteristics section for burst and tran-
sient response waveforms.
C
CSS
= 1000pF
C
CSS
= 0.01µF
C
CSS
= 0.1µF

LT3435EFE#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 500kHz Version of LT3434 (200kHz)
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
Payment:
T/T Paypal Visa MoneyGram Western Union