LT3667
18
3667fb
For more information www.linear.com/LT3667
APPLICATIONS INFORMATION
This simple design guide will not always result in the
optimum inductor selection for a given application. As a
general rule, lower output voltages and higher switching
frequency will require smaller inductor values. If the ap
-
plication requires
less than 400mA load current, then a
lesser inductor value may be acceptable. This allows the
use of a physically smaller inductor, or one with a lower
DCR resulting in higher efficiency. However, the inductance
should in general not be smaller than 10µH.
Be aware that if the inductance differs from the simple
rule above, then the maximum load current will depend
on input voltage. In addition, low inductance may result
in discontinuous mode operation, which further reduces
maximum load current. For details of maximum output
current and discontinuous mode operation, see Linear
Technology’s Application Note 44. Finally, for duty cycles
greater than 50% (V
OUT1
/V
IN1
> 0.5), a minimum inductance
is required to avoid sub-harmonic oscillations:
L
MIN
= V
OUT1
+ V
D
( )
•
f
SW
where f
SW
is the switching frequency in MHz, V
OUT1
is
the output voltage, V
D
is the catch diode drop (~0.5V)
and L
MIN
is the inductor value in µH.
Catch Diode
The catch diode (D1 from block diagram) conducts current
only during switch off-time. Use a 1A Schottky diode for
best performance.
Peak reverse voltage is equal to V
IN1
if it is below the
overvoltage protection threshold. This feature keeps the
switch off for V
IN1
> OVLO (44V maximum). For inputs up
to the maximum operating voltage of 40V, use a diode with
a reverse voltage rating greater than the input voltage. If
transients at the input of up to 60V are expected, use a diode
with a reverse voltage rating only higher than the maximum
OVLO of 44V. If operating at high ambient temperatures,
consider using a Schottky with low reverse leakage. For
example, Diodes Inc. SBR1U40LP or DFLS160, ON Semi
MBRM140, and Central Semiconductor CMMSH1-60 are
good choices for the catch diode.
Input Capacitor
Bypass the input of the LT3667 circuit with a ceramic
capacitor of X7R or X5R type. Y5V types have poor
performance over temperature and applied voltage,
and
should
not be used. A 1μF to 4.7μF ceramic capacitor is
adequate to bypass the LT3667 and will easily handle
the ripple current. Note that a larger input capacitance
is required when a lower switching frequency is used
(due to longer on-times). If the input power source has
high impedance, or there is significant inductance due to
long wires or cables, additional bulk capacitance may be
necessary. This can be provided with a low performance
electrolytic capacitor. Step-down regulators draw current
from the input supply in pulses with very fast rise and
fall times. The input capacitor is required to reduce the
resulting voltage ripple at the LT3667 and to force this
very high frequency switching current into a tight local
loop, minimizing EMI. A 1μF capacitor is capable of this
task, but only if it is placed close to the LT3667 (see the
PCB Layout section). A second precaution regarding the
ceramic input capacitor concerns the maximum input
voltage rating of the LT3667. A ceramic input capacitor
combined with trace or cable inductance forms a high
quality (under damped) tank circuit. If the LT3667 circuit
is plugged into a live supply, the input
voltage can ring to
twice its nominal value, possibly exceeding the LT3667’s
voltage rating. This situation is easily avoided (see the Hot
Plugging Safely section).
Output Capacitor and Output Ripple
The output capacitor has two essential functions. Along
with the inductor, it filters the square wave generated
by the LT3667 to produce the DC output. In this role it
determines the output ripple, and low impedance at the
switching frequency is important. The second function
is to store energy in order to satisfy transient loads and
stabilize the switching regulator’s control loop. Ceramic
capacitors have very low equivalent series resistance
(ESR) and provide the best ripple performance. A good
starting value is:
C
OUT1
=
V
OUT1
• f
SW