LTC3411
10
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higher ripple current which causes this to occur at lower
load currents. This causes a dip in effi ciency in the upper
range of low current operation. In Burst Mode operation,
lower inductance values will cause the burst frequency
to increase.
Inductor Core Selection
Different core materials and shapes will change the
size/current and price/current relationship of an induc-
tor. Toroid or shielded pot cores in ferrite or permalloy
materials are small and don’t radiate much energy, but
generally cost more than powdered iron core inductors
with similar electrical characteristics. The choice of which
style inductor to use often depends more on the price vs
size requirements and any radiated fi eld/EMI requirements
than on what the LTC3411 requires to operate. Table 1
shows some typical surface mount inductors that work
well in LTC3411 applications.
Table 1. Representative Surface Mount Inductors
MANU-
FACTURER PART NUMBER VALUE
MAX DC
CURRENT DCR HEIGHT
Toko A914BYW-2R2M-D52LC 2.2μH 2.05A 49mΩ 2mm
Toko A915AY-2ROM-D53LC 2μH 3.3A 22mΩ 3mm
Coilcraft D01608C-222 2.2μH 2.3A 70mΩ 3mm
Coilcraft LP01704-222M 2.2μH 2.4A 120mΩ 1mm
Sumida CDRH4D282R2 2.2μH 2.04A 23mΩ 3mm
Sumida CDC5D232R2 2.2μH 2.16A 30mΩ 2.5mm
Taiyo Yuden N06DB2R2M 2.2μH 3.2A 29mΩ 3.2mm
Taiyo Yuden N05DB2R2M 2.2μH 2.9A 32mΩ 2.8mm
Murata LQN6C2R2M04 2.2μH 3.2A 24mΩ 5mm
Catch Diode Selection
Although unnecessary in most applications, a small
improvement in effi ciency can be obtained in a few ap-
plications by including the optional diode D1 shown in
Figure 5, which conducts when the synchronous switch is
off. When using Burst Mode operation or pulse skip mode,
the synchronous switch is turned off at a low current and
the remaining current will be carried by the optional diode.
It is important to adequately specify the diode peak cur-
rent and average power dissipation so as not to exceed
the diode ratings. The main problem with Schottky diodes
is that their parasitic capacitance reduces the effi ciency,
usually negating the possible benefi ts for LTC3411 circuits.
Another problem that a Schottky diode can introduce is
higher leakage current at high temperatures, which could
reduce the low current effi ciency.
Remember to keep lead lengths short and observe proper
grounding (see Board Layout Considerations) to avoid ring-
ing and increased dissipation when using a catch diode.
Input Capacitor (C
IN
) Selection
In continuous mode, the input current of the converter is a
square wave with a duty cycle of approximately V
OUT
/V
IN
.
To prevent large voltage transients, a low equivalent series
resistance (ESR) input capacitor sized for the maximum
RMS current must be used. The maximum RMS capacitor
current is given by:
II
VVV
V
RMS MAX
OUT IN OUT
IN
()
APPLICATIONS INFORMATION
LTC3411
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where the maximum average output current I
MAX
equals
the peak current minus half the peak-to-peak ripple cur-
rent, I
MAX
= I
LIM
ΔI
L
/2.
This formula has a maximum at V
IN
= 2V
OUT
, where
I
RMS
= I
OUT
/2. This simple worst case is commonly used
to design because even signifi cant deviations do not offer
much relief. Note that capacitor manufacturers ripple cur-
rent ratings are often based on only 2000 hours lifetime.
This makes it advisable to further derate the capacitor,
or choose a capacitor rated at a higher temperature than
required. Several capacitors may also be paralleled to
meet the size or height requirements of the design. An
additional 0.1μF to 1μF ceramic capacitor is also recom-
mended on V
IN
for high frequency decoupling, when not
using an all ceramic capacitor solution.
Output Capacitor (C
OUT
) Selection
The selection of C
OUT
is driven by the required ESR to
minimize voltage ripple and load step transients. Typically,
once the ESR requirement is satisfi ed, the capacitance
is adequate for fi ltering. The output ripple (ΔV
OUT
) is
determined by:
Δ≈Δ +
V I ESR
fC
OUT L
O OUT
1
8
where f = operating frequency, C
OUT
= output capacitance
and ΔI
L
= ripple current in the inductor. The output ripple
is highest at maximum input voltage since ΔI
L
increases
with input voltage. With ΔI
L
= 0.3 • I
LIM
the output ripple
will be less than 100mV at maximum V
IN
and f
O
= 1MHz
with:
ESRC
OUT
< 150mΩ
Once the ESR requirements for C
OUT
have been met, the
RMS current rating generally far exceeds the I
RIPPLE(P-P)
requirement, except for an all ceramic solution.
In surface mount applications, multiple capacitors may
have to be paralleled to meet the capacitance, ESR or RMS
current handling requirement of the application. Aluminum
electrolytic, special polymer, ceramic and dry tantulum
capacitors are all available in surface mount packages.
The OS-CON semiconductor dielectric capacitor avail-
able from Sanyo has the lowest ESR(size) product of any
aluminum electrolytic at a somewhat higher price. Special
polymer capacitors, such as Sanyo POSCAP, offer very
low ESR, but have a lower capacitance density than other
types. Tantalum capacitors have the highest capacitance
density, but it has a larger ESR and it is critical that the
capacitors are surge tested for use in switching power
supplies. An excellent choice is the AVX TPS series of
surface mount tantalums, avalable in case heights ranging
from 2mm to 4mm. Aluminum electrolytic capacitors have
a signifi cantly larger ESR, and is often used in extremely
cost-sensitive applications provided that consideration
is given to ripple current ratings and long term reliability.
Ceramic capacitors have the lowest ESR and cost but also
have the lowest capacitance density, a high voltage and
temperature coeffi cient and exhibit audible piezoelectric
effects. In addition, the high Q of ceramic capacitors along
with trace inductance can lead to signifi cant ringing. Other
capacitor types include the Panasonic specialty polymer
(SP) capacitors.
In most cases, 0.1μF to 1μF of ceramic capacitors should
also be placed close to the LTC3411 in parallel with the
main capacitors for high frequency decoupling.
APPLICATIONS INFORMATION
LTC3411
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Ceramic Input and Output Capacitors
Higher value, lower cost ceramic capacitors are now be-
coming available in smaller case sizes. These are tempting
for switching regulator use because of their very low ESR.
Unfortunately, the ESR is so low that it can cause loop
stability problems. Solid tantalum capacitor ESR generates
a loop “zero” at 5kHz to 50kHz that is instrumental in giving
acceptable loop phase margin. Ceramic capacitors remain
capacitive to beyond 300kHz and ususally resonate with
their ESL before ESR becomes effective. Also, ceramic
caps are prone to temperature effects which requires the
designer to check loop stability over the operating tem-
perature range. To minimize their large temperature and
voltage coeffi cients, only X5R or X7R ceramic capacitors
should be used. A good selection of ceramic capacitors
is available from Taiyo Yuden, TDK and Murata.
Great care must be taken when using only ceramic input
and output capacitors. When a ceramic capacitor is used
at the input and the power is being supplied through long
wires, such as from a wall adapter, a load step at the output
can induce ringing at the V
IN
pin. At best, this ringing can
couple to the output and be mistaken as loop instability.
At worst, the ringing at the input can be large enough to
damage the part.
Since the ESR of a ceramic capacitor is so low, the input
and output capacitor must instead fulfi ll a charge storage
requirement. During a load step, the output capacitor must
instantaneously supply the current to support the load
until the feedback loop raises the switch current enough
to support the load. The time required for the feedback
loop to respond is dependent on the compensation com-
ponents and the output capacitor size. Typically, 3 to 4
cycles are required to respond to a load step, but only in
the fi rst cycle does the output drop linearly. The output
droop, V
DROOP
, is usually about 2 to 3 times the linear
drop of the fi rst cycle. Thus, a good place to start is with
the output capacitor size of approximately:
C
I
fV
OUT
OUT
O DROOP
Δ
25.
More capacitance may be required depending on the duty
cycle and load step requirements.
In most applications, the input capacitor is merely required
to supply high frequency bypassing, since the impedance
to the supply is very low. A 10μF ceramic capacitor is
usually enough for these conditions.
Setting the Output Voltage
The LTC3411 develops a 0.8V reference voltage between
the feedback pin, V
FB
, and the signal ground as shown in
Figure 5. The output voltage is set by a resistive divider
according to the following formula:
VV
R
R
OUT
≈+
08 1
2
1
.
Keeping the current small (<5μA) in these resistors maxi-
mizes effi ciency, but making them too small may allow
stray capacitance to cause noise problems and reduce the
phase margin of the error amp loop.
To improve the frequency response, a feed-forward capaci-
tor C
F
may also be used. Great care should be taken to
route the V
FB
line away from noise sources, such as the
inductor or the SW line.
APPLICATIONS INFORMATION

LTC3411EDD#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 1.25A, 4MHz, Sync Buck DC/DC Conv
Lifecycle:
New from this manufacturer.
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