LTC1702IGN#TR Linear Technology, LTC1702IGN#TR Datasheet - Page 22

IC REG SW DUAL SYNC 2PH 24SSOP

LTC1702IGN#TR

Manufacturer Part Number
LTC1702IGN#TR
Description
IC REG SW DUAL SYNC 2PH 24SSOP
Manufacturer
Linear Technology
Series
PolyPhase®r
Type
Step-Down (Buck)r
Datasheet

Specifications of LTC1702IGN#TR

Internal Switch(s)
No
Synchronous Rectifier
Yes
Number Of Outputs
2
Current - Output
1A, 25A
Frequency - Switching
550kHz
Voltage - Input
3 ~ 7 V
Operating Temperature
-40°C ~ 85°C
Mounting Type
Surface Mount
Package / Case
24-SSOP
Lead Free Status / RoHS Status
Contains lead / RoHS non-compliant
Voltage - Output
-
Power - Output
-

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APPLICATIONS
LTC1702
“Type 3” loops (Figure 11) use two poles and two zeros to
obtain a 180° phase boost in the middle of the frequency
band. A properly designed type 3 circuit can maintain
acceptable loop stability even when low output capacitor
ESR causes the LC section to approach 180° phase shift
well above the initial LC roll-off. As with a type 2 circuit, the
loop should cross through 0dB in the middle of the phase
bump to maximize phase margin. Many LTC1702 circuits
using low ESR tantalum or OS-CON output capacitors
need type 3 compensation to obtain acceptable phase
margin with a high bandwidth feedback loop.
Feedback Component Selection
Selecting the R and C values for a typical type 2 or type 3
loop is a nontrivial task. The applications shown in this data
sheet show typical values, optimized for the power com-
ponents shown. They should give acceptable performance
with similar power components, but can be way off if even
one major power component is changed significantly.
22
GAIN
Figure 11a. Type 3 Amplifier Schematic Diagram
(dB)
Figure 11B. Type 3 Amplifier Transfer Function
0
IN
GAIN
PHASE
–6dB/OCT
C3
U
R1
R
B
R3
+6dB/OCT
INFORMATION
U
V
REF
R2
+
C2
C1
W
–6dB/OCT
1702 F11a
OUT
PHASE
0
–90
–180
–270
1702 F11b
(DEG)
U
Applications that require optimized transient response will
need to recalculate the compensation values specifically
for the circuit in question. The underlying mathematics are
complex, but the component values can be calculated in a
straightforward manner if we know the gain and phase of
the modulator at the crossover frequency.
Modulator gain and phase can be measured directly from
a breadboard, or can be simulated if the appropriate
parasitic values are known. Measurement will give more
accurate results, but simulation can often get close enough
to give a working system. To measure the modulator gain
and phase directly, wire up a breadboard with an LTC1702
and the actual MOSFETs, inductor, and input and output
capacitors that the final design will use. This breadboard
should use appropriate construction techniques for high
speed analog circuitry: bypass capacitors located close to
the LTC1702, no long wires connecting components,
appropriately sized ground returns, etc. Wire the feedback
amplifier as a simple type 1 loop, with a 10k resistor from
V
FB. Choose the bias resistor (R
desired output voltage. Disconnect R
connect it to a signal generator or to the source output of
a network analyzer (Figure 12) to inject a test signal into
the loop. Measure the gain and phase from the COMP pin
to the output node at the positive terminal of the output
capacitor. Make sure the analyzer’s input is AC coupled so
that the DC voltages present at both the COMP and V
ANALYZER
ANALYZER
OUT
SOURCE
V
FROM
COMP
Figure 12. Modulator Gain/Phase Measurement Set-Up
TO
AC
to FB and a 0.1µF feedback capacitor from COMP to
10µF
0.1µF
R
+
B
10k
NC
COMP
FB
RUN/SS
SGND PGND
V
1/2 LTC1702
CC
10Ω
BOOST2
PV
FAULT
CC
FCB
MBR0530T
SW
BG
TG
B
) as required to set the
5V
QT
QB
+
B
from ground and
C
1µF
IN
L
EXT
1702 F12
+
C
V
TO
ANALYZER
OUT
OUT
1702fa
OUT

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