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LTC3548EDD-2-TRPBF Просмотр технического описания (PDF) - Linear Technology

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LTC3548EDD-2-TRPBF Datasheet PDF : 16 Pages
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LTC3548-2
APPLICATIONS INFORMATION
A general LTC3548-2 application circuit is shown in
Figure 2. External component selection is driven by the
load requirement, and begins with the selection of the
inductor L. Once the inductor is chosen, CIN and COUT
can be selected.
VIN
2.5V TO 5.5V
VOUT2
CIN
BM*
PS*
RUN2 VIN
MODE/SYNC
RUN1
POR
L2
C5
LTC3548-2
SW2
SW1
R5
POWER-ON
RESET
L1
VOUT1
R2
COUT2
VFB2
R1
VOUT1
GND
COUT1
35482 F02
*MODE/SYNC = 0V: PULSE SKIPPING
MODE/SYNC = VIN: Burst Mode OPERATION
Figure 2. LTC3548-2 General Schematic
Inductor Selection
Although the inductor does not influence the operating fre-
quency, the inductor value has a direct effect on ripple cur-
rent. The inductor ripple current ΔIL decreases with higher
inductance and increases with higher VIN or VOUT:
ΔIL
=
VOUT
fO • L
⎝⎜1–
VOUT
VIN
⎠⎟
Accepting larger values of ΔIL allows the use of low
inductances, but results in higher output voltage ripple,
greater core losses, and lower output current capability.
A reasonable starting point for setting ripple current is
ΔIL = 0.3 • IOUT(MAX), where IOUT(MAX) is 800mA for channel 1
and 400mA for channel 2. The largest ripple current ΔIL
occurs at the maximum input voltage. To guarantee that
the ripple current stays below a specified maximum, the
inductor value should be chosen according to the follow-
ing equation:
L
VOUT
fO ΔIL
1–
VOUT
VIN(MAX)
The inductor value will also have an effect on Burst Mode
operation. The transition from low current operation
begins when the peak inductor current falls below a level
set by the burst clamp. Lower inductor values result in
higher ripple current which causes this to occur at lower
load currents. This causes 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.
Toroid or shielded pot cores in ferrite or permalloy
materials are small and do not radiate much energy,
but generally cost more than powdered iron core induc-
tors with similar electrical characteristics. The choice of
which style inductor to use often depends more on the
price vs size requirements and any radiated field/EMI
requirements than on what the LTC3548-2 requires to
operate. Table 1 shows some typical surface mount
inductors that work well in LTC3548-2 applications.
Table 1. Representative Surface Mount Inductors
PART
NUMBER
VALUE DCR
MAX DC
SIZE
(μH) (Ω MAX) CURRENT (A) W × L × H (mm3)
Sumida
2.2
0.075
CDRH3D16
3.3
0.110
4.7
0.162
1.20
3.8 × 3.8 × 1.8
1.10
0.90
Sumida
1.5
0.068
CDRH2D11
2.2
0.170
0.900
0.780
3.2 × 3.2 × 1.2
Sumida
CMD4D11
2.2
0.116
3.3
0.174
0.950
0.770
4.4 × 5.8 × 1.2
Murata
LQH32CN
1.0
0.060
2.2
0.097
1.00
2.5 × 3.2 × 2.0
0.79
Toko
D312F
2.2
0.060
3.3
0.260
1.08
2.5 × 3.2 × 2.0
0.92
Panasonic
3.3
0.17
ELT5KT
4.7
0.20
1.00
4.5 × 5.4 × 1.2
0.95
Input Capacitor (CIN) Selection
In continuous mode, the input current of the converter is a
square wave with a duty cycle of approximately VOUT/VIN.
To prevent large voltage transients, a low equivalent series
resistance (ESR) input capacitor sized for the maximum
35482fb
8

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