LT1765/LT1765-1.8/LT1765-2.5/
LT1765-3.3/LT1765-5
13
1765fd
APPLICATIONS INFORMATION
Example: with V
IN
= 10V, V
OUT
= 5V and I
OUT
= 2A:
P
W
PW
PW
SW
BOOST
Q
=
( )()()
+
()
()( )
()
=+ =
=
()( )
=
=
()
=
013 2 5
10
17 10 2 10 1 25 10
026 043 069
5250
10
01
10 0 001 0 01
2
96
2
.
•.
...
/
.
..
Total power dissipation, P
TOT
, is 0.69 + 0.1 + 0.01 = 0.8W.
Thermal resistance for the LT1765 16-lead TSSOP exposed
pad package is infl uenced by the presence of internal or
backside planes. With a full plane under the package,
thermal resistance will be about 45°C/W. With no plane
under the package, thermal resistance will increase to
about 110°C/W. For the exposed pad package θ
JC(PAD)
=
10°C/W. Thermal resistance is dominated by board perfor-
mance. To calculate die temperature, use the appropriate
thermal resistance number and add in worst-case ambient
temperature:
T
J
= T
A
+ θ
JA (PTOT)
When estimating ambient, remember the nearby catch
diode will also be dissipating power.
P
VV V I
V
DIODE
F IN OUT LOAD
IN
=
()
()()
V
F
= Forward voltage of diode (assume 0.5V at 2A)
PW
DIODE
=
()
()()
=
05 10 5 2
10
05
.
.
Notice that the catch diode’s forward voltage contributes
a signifi cant loss in the overall system effi ciency. A larger,
lower V
F
diode can improve effi ciency by several percent.
Typical thermal resistance of the board θ
B
is 35°C/W. At
an ambient temperature of 25°C,
T
J
= T
A
+ θ
JA
(P
TOT
) + θ
B
(P
DIODE
)
T
J
= 25 + 45 (0.8) + 35 (0.5) = 79°C
DIE TEMPERATURE MEASUREMENT
If a true die temperature is required, a measurement of the
SYNC to GND pin resistance can be used. The SYNC pin
resistance across temperature must fi rst be calibrated, with
no signifi cant output load, in an oven. An initial value of
40k with a temperature coeffi cient of 0.16%/°C is typical.
The same measurement can then be used in operation to
indicate the die temperature.
FREQUENCY COMPENSATION
Before starting on the theoretical analysis of frequency
response, the following should be remembered—the worse
the board layout, the more diffi cult the circuit will be to
stabilize. This is true of almost all high frequency analog
circuits, read the ‘LAYOUT CONSIDERATIONS’ section fi rst.
Common layout errors that appear as stability problems
are distant placement of input decoupling capacitor and/or
catch diode, and connecting the V
C
compensation to a
ground track carrying signifi cant switch current. In addition,
the theoretical analysis considers only fi rst order ideal
component behavior. For these reasons, it is important
that a fi nal stability check is made with production layout
and components.
The LT1765 uses current mode control. This alleviates many
of the phase shift problems associated with the inductor.
The basic regulator loop is shown in Figure 7, with both
tantalum and ceramic capacitor equivalent circuits. The
LT1765 can be considered as two g
m
blocks, the error
amplifi er and the power stage.
Figure 7. Model for Loop Response
+
1.2V
V
SW
V
C
LT1765
GND
1765 F07
R1
OUTPUT
ESR
C
F
C
C
R
C
500k
ERROR
AMPLIFIER
FB
R2
C1
CURRENT MODE
POWER STAGE
g
m
= 5mho
g
m
=
850
μmho
+
ESL
CERAMICTANTALUM
C1
LT1765/LT1765-1.8/LT1765-2.5/
LT1765-3.3/LT1765-5
14
1765fd
APPLICATIONS INFORMATION APPLICATIONS INFORMATION
Figure 8 shows the overall loop response with a 330pF VC
capacitor and a typical 100μF tantalum output capacitor.
The response is set by the following terms:
Error amplifi er:
DC gain set by g
m
and R
L
= 850μ • 500k = 425.
Pole set by C
F
and R
L
= (2π • 500k • 330p)
–1
= 965Hz.
Unity-gain set by C
F
and g
m
= (2π • 330p • 850μ
–1
)
–1
=
410kHz.
Power stage:
DC gain set by g
m
and R
L
(assume 5Ω) = 5 • 5 = 25.
Pole set by C
OUT
and R
L
= (2π • 100μ • 10)
–1
= 159Hz.
Unity-gain set by C
OUT
and g
m
= (2π • 100μ • 5
–1
)
–1
=
8kHz.
Tantalum output capacitor:
Zero set by C
OUT
and C
ESR
= (2π • 100μ • 0.1)
–1
= 15.9kHz.
The zero produced by the ESR of the tantalum output capaci-
tor is very useful in maintaining stability. Ceramic output
capacitors do not have a zero due to very low ESR, but are
dominated by their ESL. They form a notch in the 1MHz to
10MHz range. Without this zero, the V
C
pole must be made
dominant. A typical value of 2.2nF will achieve this.
If better transient response is required, a zero can be
added to the loop using a resistor (R
C
) in series with the
compensation capacitor. As the value of R
C
is increased,
transient response will generally improve, but two effects
limit its value. First, the combination of output capacitor
ESR and a large R
C
may stop loop gain rolling off altogether.
Second, if the loop gain is not rolled suffi ciently at the
switching frequency, output ripple will perturb the V
C
pin
enough to cause unstable duty cycle switching similar
to subharmonic oscillation. This may not be apparent
at the output. Small signal analysis will not show this
since a continuous time system is assumed. If needed,
an additional capacitor (C
F
) can be added to the V
C
pin to
form a pole at typically one fi fth the switching frequency
(If R
C
= ~ 5k, C
F
= ~ 100pF)
When checking loop stability, the circuit should be operated
over the application’s full voltage, current and temperature
range. Any transient loads should be applied and the output
voltage monitored for a well-damped behavior.
CONVERTER WITH BACKUP OUTPUT REGULATOR
In systems with a primary and backup supply, for example,
a battery powered device with a wall adapter input, the
output of the LT1765 can be held up by the backup supply
with its input disconnected. In this condition, the SW pin
will source current into the V
IN
pin. If the SHDN pin is held
at ground, only the shutdown current of 6μA will be pulled
via the SW pin from the second supply. With the SHDN pin
oating, the LT1765 will consume its quiescent operating
current of 1mA. The V
IN
pin will also source current to
any other components connected to the input line. If this
load is greater than 10mA or the input could be shorted to
ground, a series Schottky diode must be added, as shown
in Figure 9. With these safeguards, the output can be held
at voltages up to the V
IN
absolute maximum rating.
BUCK CONVERTER WITH ADJUSTABLE SOFT-START
Large capacitive loads or high input voltages can cause
high input currents at start-up. Figure 10 shows a circuit
that limits the dv/dt of the output at start-up, controlling
the capacitor charge rate. The buck converter is a typical
confi guration with the addition of R3, R4, C
SS
and Q1. As
the output starts to rise, Q1 turns on, regulating switch
current via the V
C
pin to maintain a constant dv/dt at the
output. Output rise time is controlled by the current through
C
SS
defi ned by R4 and Q1’s V
BE
. Once the output is in
regulation, Q1 turns off and the circuit operates normally.
R3 is transient protection for the base of Q1.
Figure 8. Overall Loop Response
FREQUENCY (Hz)
GAIN (dB)
80
60
40
20
0
–20
–40
PHASE (DEG)
180
150
120
90
60
30
0
1765 F08
GAIN
PHASE
V
OUT
= 5V
C
OUT
= 100μF, 0.1Ω
C
C
= 330pF
R
C
/C
F
= 0
I
LOAD
= 1A
10 1k 10k 1M100 100k
LT1765/LT1765-1.8/LT1765-2.5/
LT1765-3.3/LT1765-5
15
1765fd
APPLICATIONS INFORMATION
Figure 10. Buck Converter with Adjustable Soft Start
BOOST
LT1765-5
V
IN
OUTPUT
5V
2.5A
INPUT
12V
1765 F10
C2
0.18μF
C1
100μF
C
SS
15nF
C
C
330pF
D1
C3
2.2μF
D2
CMDSH-3
L1
5μH
R3
2k
V
SW
FB
SHDN
GND
V
C
SYNC
+
R4
47k
Q1
D1: B220A
Q1: 2N3904
RiseTime
RC V
V
SS OUT
BE
=
()( )( )
()
4
Using the values shown in Figure 10,
RiseTime ms==
(• )( )()
.
47 10 15 10 5
07
5
39
The ramp is linear and rise times in the order of 100ms are
possible. Since the circuit is voltage controlled, the ramp
rate is unaffected by load characteristics and maximum
output current is unchanged. Variants of this circuit can
be used for sequencing multiple regulator outputs.
Dual Output Converter
The circuit in Figure 11 generates both positive and negative
5V outputs with a single piece of magnetics. The two induc-
tors shown are actually just two windings on a standard
B H Electronics inductor. The topology for the 5V output
is a standard buck converter. The –5V topology would be
a simple fl yback winding coupled to the buck converter
if C4 were not present. C4 creates a SEPIC (single-ended
primary inductance converter) topology which improves
regulation and reduces ripple current in L1. Without C4,
the voltage swing on L1B compared to L1A would vary
due to relative loading and coupling losses. C4 provides a
low impedance path to maintain an equal voltage swing in
L1B, improving regulation. In a fl yback converter, during
switch on time, all the converters energy is stored in L1A
only, since no current fl ows in L1B. At switch off, energy
is transferred by magnetic coupling into L1B, powering
the –5V rail. C4 pulls L1B positive during switch on time,
causing current to fl ow, and energy to build in L1B and
C4. At switch off, the energy stored in both L1B and C4
supply the –5V rail. This reduces the current in L1A and
changes L1B current waveform from square to triangular.
For details on this circuit, including maximum output cur-
rents, see Design Note 100
Figure 9. Dual Source Supply with 6μA Reverse Leakage
3.3V, 2A
* ONLY REQUIRED IF ADDITIONAL LOADS ON THE INPUT CAN SINK >10mA
REMOVABLE
INPUT
0.18μF
2.2nF
83k
B220A
1765 F09
2.2μF
MBRS330T3*
CMDSH-3
5μH
4.7μF
BOOST
LT1765-3.3
V
IN
V
SW
FBSHDN
GND
V
C
SYNC
ALTERNATE
SUPPLY
28.5k

LT1765EFE#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Mono 3A, 1.25MHz Buck Sw Regs
Lifecycle:
New from this manufacturer.
Delivery:
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