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Table 2. component manufacturers – Rainbow Electronics MAX1641 User Manual

Page 9

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where V

TERM

= 2V and V

OUT

is the desired output

voltage.

Programming the Off-Time

When programming the off-time, consider such factors
as maximum inductor current ripple, maximum output
voltage, inductor value, and inductor current rating. The
output current ripple is less than the inductor current rip-
ple and depends heavily on the output capacitor’s size.

Perform the following steps to program the off-time:

1) Select the maximum output current ripple. I

R

(A)

2) Select the maximum output voltage. V

OUT

(MAX)(V)

3) Calculate the inductor value range as follows:

L

MIN

= (V

OUTMAX

x 1µs) / I

R

L

MAX

= (V

OUTMAX

x 10µs) / I

R

4) Select an inductor value in this range.

5) Calculate t

OFF

as follows:

6) Program t

OFF

by selecting R

TOFF

from:

R

TOFF

= (29.3 x 10

9

) x t

OFF

7) Calculate the switching frequency by:

fs = 1 / (t

ON

+ t

OFF

)

where t

ON

= (I

R

x L) / (V

IN

- V

OUT

) and I

R

= (V

OUT

x

t

OFF

) / L. L is the inductor value, V

IN

is the input volt-

age, V

OUT

is the output voltage, and I

R

is the output

peak-to-peak current ripple.

Note that R

TOFF

sets both the off-time and the pulse-

trickle charge period.

Reference

The on-chip reference is laser trimmed for a precise 2V
at REF. REF can source no more than 50µA. Bypass
REF with a 0.1µF capacitor to ground.

Constant-Current Loop: AC Loop

Compensation

The constant-current loop’s output is brought out at CC.
To reduce noise due to variations in switching currents,
bypass CC with a 1nF to 100nF capacitor to ground. A
large capacitor value maintains a constant average out-
put current but slows the loop response to changes in
switching current. A small capacitor value speeds up
the loop response to changes in switching current,

generating increased ripple at the output. Select C

CC

to optimize the ripple vs. loop response.

Synchronous Rectification

Synchronous rectification reduces conduction losses in
the rectifier by shunting the Schottky diode with a low-
resistance MOSFET switch. In turn, efficiency increases
by about 3% to 5% at heavy loads. To prevent cross-
conduction or “shoot-through,” the synchronous rectifier
turns on shortly after the P-channel power MOSFET

turns off. The synchronous rectifier remains off for 90%
of the off-time. In low-cost designs, the synchronous
rectifier FET may be replaced by a Schottky diode.

Component Selection

External Switching Transistors

The MAX1640/MAX1641 drive an enhancement-mode
P-channel MOSFET and a synchronous-rectifier N-
channel MOSFET (Table 2).

When selecting a P-channel FET, some important para-
meters to consider are on-resistance (r

DS(ON)

), maxi-

mum drain-to-source voltage (V

DS

max), maximum

gate-to-source voltage (V

GS

max), and minimum

threshold voltage (V

TH

min).

In high-current applications, MOSFET package power
dissipation often becomes a dominant design factor.
I2R power losses are the greatest heat contributor for
both high-side and low-side MOSFETs. Switching loss-
es affect the upper MOSFET only (P-channel), since the
Schottky rectifier or the N-FET body diode clamps the
switching node before the synchronous rectifier turns on.

Rectifier Diode

If an N-channel MOSFET synchronous rectifier is not
used, a Schottky rectifier is needed. The MAX1640/

t

=

L x I

V

OFF

R

OUTMAX

MAX1640/MAX1641

Adjustable-Output, Switch-Mode

Current Source with Synchronous Rectifier

_______________________________________________________________________________________

9

Table 2. Component Manufacturers

COMPONENT

MANUFACTURER

MOSFETs

Sense Resistor

Capacitors

International Rectifier

Dale

AVX

Sumida

Coilcraft

Inductor

Coiltronics

Siliconix

S14539DY

IRF7309

WSL-2010 series

TPS series

MBAR5340t3

CDRH125 series

D03316P series

UP2 series

IRC

LR2010-01 series

Sprague

595D series

Nihon

NSQ03A04

Rectifier

IN5817-IN5822

Motorola