LTC3405A-1.5 datasheet(8/16 Pages) LINER

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LTC3405A-1.5/LTC3405A-1.8

sn3405a1518 3405a1518fs

APPLICATIO S I FOR ATIO

Table 1. Representative Surface Mount Inductors

MAX DC

MANUFACTURER PART NUMBER

VALUE CURRENT DCR HEIGHT

Taiyo Yuden

LB2016T2R2M

2.2

µH 315mA 0.13Ω 1.6mm

LB2012T2R2M

2.2

µH 240mA 0.23Ω 1.25mm

LB2016T3R3M

3.3

µH 280mA

0.2

Ω 1.6mm

Panasonic

ELT5KT4R7M

4.7

µH 950mA

0.2

Ω 1.2mm

Murata

LQH32CN2R2M33 4.7

µH 450mA

0.2

Ω 2mm

Taiyo Yuden

LB2016T4R7M

4.7

µH 210mA 0.25Ω 1.6mm

Panasonic

ELT5KT6R8M

6.8

µH 760mA

0.3

Ω 1.2mm

Panasonic

ELT5KT100M

µH

680mA

0.36

Ω 1.2mm

Sumida

CMD4D116R8MC 6.8

µH 620mA 0.23Ω 1.2mm

The basic LTC3405A series parts application circuit is

shown in Figure 1. External component selection is driven

by the load requirement and begins with the selection of L

followed by CIN and COUT.

Inductor Selection

For most applications, the inductor value will fall in the

range of 2.2

µH to 10µH. Its value is determined by the

desired ripple current. Large value inductors lower ripple

current and small value inductors result in higher ripple

currents. Higher VIN or VOUT also increases the ripple

current as shown in equation 1. A reasonable starting point

for setting ripple current is

∆IL = 120mA (40% of 300mA).

∆= ()( )

−









OUT

(1)

The DC current rating of the inductor should be at least

equal to the maximum load current plus half the ripple

current to prevent core saturation. Thus, a 360mA rated

inductor should be enough for most applications (300mA

+ 60mA). For better efficiency, choose a low DC-resistance

inductor.

The inductor value also has an effect on Burst Mode

operation. The transition to low current operation begins

when the inductor current peaks fall to approximately

100mA. Lower inductor values (higher

∆IL) will cause this

to occur at lower load currents, which can cause a dip in

efficiency 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 inductor. Tor-

oid 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 induc-

tor to use often depends more on the price vs size require-

ments and any radiated field/EMI requirements than on

what the LTC3405A series parts require to operate. Table

1 shows some typical surface mount inductors that work

well in LTC3405A series parts applications.

CIN and COUT Selection

In continuous mode, the source current of the top MOSFET

is a square wave of duty cycle VOUT/VIN. To prevent large

voltage transients, a low ESR input capacitor sized for the

maximum RMS current must be used. The maximum

RMS capacitor current is given by:

OMAX

OUT

required IRMS ≅

−

()

[]12/

This formula has a maximum at VIN = 2VOUT, where

IRMS = IOUT/2. This simple worst-case condition is com-

monly used for design because even significant deviations

do not offer much relief. Note that the capacitor

manufacturer’s ripple current ratings are often based on

2000 hours of life. This makes it advisable to further derate

the capacitor, or choose a capacitor rated at a higher

temperature than required. Always consult the manufac-

turer if there is any question.

The selection of COUT is driven by the required effective

series resistance (ESR). Typically, once the ESR require-

ment for COUT has been met, the RMS current rating

generally far exceeds the IRIPPLE(P-P) requirement. The

output ripple

∆VOUT is determined by:

∆≅ ∆









I ESR

OUT

where f = operating frequency, COUT = output capacitance

and

∆IL = ripple current in the inductor. For a fixed output

voltage, the output ripple is highest at maximum input

voltage since

∆IL increases with input voltage.

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