LTC3416
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APPLICATIO S I FOR ATIO
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coincidentally or ratiometrically track another output volt-
age as shown in Figure 3.
If the voltage on the TRACK pin is less than 0.8V, voltage
tracking is enabled. During voltage tracking, the output
voltage regulates to the tracking voltage through a resistor
divider network. The output voltage during tracking can be
calculated with the following equation:
VV
R
R
OUT TRACK
=+
1
2
1
, V
TRACK
< 0.8V
Voltage tracking can be accomplished by sensing a frac-
tion of the output voltage from another regulator. This is
typically done by using a resistor divider to attenuate the
output voltage that is being tracked. Setting this attenua-
tion factor equal to the reciprocal of the gain factor
provided by the feedback resistors will force the regulator
outputs to be equal to each other during tracking. If
tracking is not desired, connect the TRACK pin to SV
IN
.
To implement the coincident tracking shown in Figure 3a,
connect an extra resistor divider to the output of V
OUT2
and
connect its midpoint to the TRACK pin of the LTC3416 as
shown in Figure 4. The ratio of this divider should be
selected the same as that of V
OUT1
’s resistor divider. To
implement the ratiometric sequencing in Figure 3b, the
extra resistor divider’s ratio should be set so that the
TRACK pin voltage exceeds 1.05V by the end of the start-
up period. The LTC3416 utilizes a method in which the
TRACK pin’s control over the output voltage is gradually
released as the TRACK pin voltage approaches 0.8V. With
this technique, some overdrive will be required on the
TRACK pin to ensure that the tracking function is com-
pletely disabled at the end of the start-up period.
For coincident tracking, the following condition should be
satisfied to ensure that tracking is disabled at the end of
start-up.
V
OUT2
1.32 V
OUT1
For ratiometric tracking, the following equation can be
used to calculate the resistor values:
RR
V
V
VV
OUT
TRACK
TRACK
43 1
105
2
=
.
TIME
(3a) Coincident Tracking
V
OUT2
V
OUT1
OUTPUT VOLTAGE
TIME
3416 F03
(3b) Ratiometric Sequencing
V
OUT2
V
OUT1
OUTPUT VOLTAGE
Figure 3. Two Different Modes of Output Voltage Sequencing
Figure 4. Setup for Tracking and Ratiometric Sequencing
R4 R2
R3 R1
TO
V
FB(MASTER)
PIN
TO
TRACK
PIN
V
OUT2
3416 F04
LTC3416
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An alternative method of tracking is shown in Figure 5. For
the circuit of Figure 5, the following equations can be used
to determine the resistor values:
VV
R
R
VV
RR
R
RR
V
V
OUT
OUT
OUT
OUT
1
2
2
1
08 1
2
1
08 1
45
3
43 1
=+
=+
+
=
.
.
Soft-Start
The RUN/SS pin provides a means to shut down the
LTC3416 as well as a timer for soft-start. Pulling the RUN/
SS pin below 0.5V places the LTC3416 in a low quiescent
current shutdown state (I
Q
< 1µA).
The soft-start gradually raises the clamp on I
TH
. The full
current range becomes available on I
TH
after the voltage
on I
TH
reaches approximately 2V. The clamp on I
TH
is set
externally with a resistor and capacitor on the RUN/SS pin.
The soft-start duration can be calculated by using the
following formula:
tRCIn
V
VV
Seconds
SS SS SS
IN
IN
=
–.
()
18
Efficiency Considerations
The efficiency of a switching regulator is equal to the
output power divided by the input power times 100%. It is
often useful to analyze individual losses to determine what
is limiting the efficiency and which change would produce
the most improvement. Efficiency can be expressed as:
Efficiency = 100% – (L1 + L2 + L3 + ...)
where L1, L2, etc. are the individual losses as a percentage
of input power.
Although all dissipative elements in the circuit produce
losses, two main sources usually account for most of the
losses: V
IN
quiescent current and I
2
R losses.
The V
IN
quiescent current loss dominates the efficiency
loss at very low load currents whereas the I
2
R loss
dominates the efficiency loss at medium to high load
currents. In a typical efficiency plot, the efficiency curve at
very low load currents can be misleading since the actual
power lost is of no consequence.
1. The V
IN
quiescent current is due to two components: the
DC bias current as given in the electrical characteristics
and the internal main switch and synchronous switch
gate charge currents. The gate charge current results
from switching the gate capacitance of the internal power
MOSFET switches. Each time the gate is switched from
high to low to high again, a packet of charge dQ moves
from V
IN
to ground. The resulting dQ/dt is the current out
of V
IN
that is typically larger than the DC bias current. In
continuous mode, I
GATECHG
= f(Q
T
+ Q
B
) where Q
T
and
Q
B
are the gate charges of the internal top and bottom
switches. Both the DC bias and gate charge losses are
proportional to V
IN
and thus their effects will be more
pronounced at higher supply voltages.
2. I
2
R losses are calculated from the resistances of the
internal switches, R
SW
, and external inductor R
L
. In
continuous mode the average output current flowing
through inductor L is “chopped” between the main
switch and the synchronous switch. Thus, the series
resistance looking into the SW pin is a function of both
top and bottom MOSFET R
DS(ON)
and the duty cycle
(DC) as follows:
R
SW
= (R
DS(ON)TOP
)(DC) + (R
DS(ON)BOT
)(1 – DC)
Figure 5. Dual Voltage System with Tracking
LTC3416
SGND
R1
3416 F05
R2
V
FB
TRACK
V
OUT1
LTC3416
SLAVE
MASTER
SGND
R3
R4
R5
V
FB
V
OUT2
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APPLICATIO S I FOR ATIO
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The R
DS(ON)
for both the top and bottom MOSFETs can
be obtained from the Typical Performance Characteris-
tics curves. Thus, to obtain I
2
R losses, simply add R
SW
to R
L
and multiply the result by the square of the
average output current.
Other losses including C
IN
and C
OUT
ESR dissipative
losses and inductor core losses generally account for less
than 2% of the total loss.
In most applications, the LTC3416 does not dissipate
much heat due to its high efficiency. But in applications
where the LTC3416 is running at high ambient tempera-
ture with low supply voltage and high duty cycles, such as
in dropout, the heat dissipated may exceed the maximum
junction temperature of the part. If the junction tempera-
ture reaches approximately 150°C, both power switches
will be turned off and the SW node will become high
impedance.
To avoid the LTC3416 from exceeding the maximum
junction temperature, the user will need to do some
thermal analysis. The goal of the thermal analysis is to
determine whether the power dissipated exceeds the
maximum junction temperature of the part. The tempera-
ture rise is given by:
T
R
= (P
D
)(θ
JA
)
where P
D
is the power dissipated by the regulator and θ
JA
is the thermal resistance from the junction of the die to the
ambient temperature. For the 20-lead exposed TSSOP
package, the θ
JA
is 38°C/W.
The junction temperature, T
J
, is given by:
T
J
= T
A
+ T
R
where T
A
is the ambient temperature.
Note that at higher supply voltages, the junction tempera-
ture is lower due to reduced switch resistance (R
DS(ON)
).
To maximize the thermal performance of the LTC3416, the
Exposed Pad should be soldered to a ground plane.
Checking Transient Response
The regulator loop response can be checked by looking at
the load transient response. Switching regulators take
several cycles to respond to a step in load current.
When a load step occurs, V
OUT
immediately shifts by an
amount equal to I
LOAD
(ESR), where ESR is the effective
series resistance of C
OUT
. I
LOAD
also begins to charge or
discharge C
OUT
generating a feedback error signal used by
the regulator to return V
OUT
to its steady-state value.
During this recovery time, V
OUT
can be monitored for
overshoot or ringing that would indicate a stability prob-
lem. The I
TH
pin external components and output capaci-
tor shown in figure 1a will provide adequate compensation
for most applications.
Design Example
As a design example, consider using the LTC3416 in an
application with the following specifications: V
IN
= 3.3V,
V
OUT1
= 1.8V, V
OUT2
= 2.5V, I
OUT1(MAX)
= I
OUT2(MAX)
= 4A,
f = 1MHz. V
OUT1
and V
OUT2
must track when powering up
and powering down.
First, calculate the timing resistor:
Rkk
OSC
==
308 10
110
10 298
11
6
.•
Use a standard value of 294k. Next, calculate the induc-
tor values for about 40% ripple current:
L
V
MHz A
V
V
H
L
V
MHz A
V
V
H
1
18
116
1
18
33
051
2
25
116
1
25
33
038
=
=
.
•.
.
.
.
.
•.
.
.
.
Using a 0.47µH inductor for both results in maximum
ripple currents of:
=
µ
=
=
µ
=
I
V
MHz H
V
V
A
I
V
MHz H
V
V
A
L
L
1
2
18
1047
1
18
33
174
25
1047
1
25
33
129
.
•.
.
.
.
.
•.
.
.
.
C
OUT1
and C
OUT2
will be selected based on the ESR that is
required to satisfy the output voltage ripple requirement
and the bulk capacitance needed for loop stability. For this
design, two 100µF ceramic capacitors will be used at each
output.

LTC3416EFE#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 4A, 4MHz, Mono Sync Buck Reg w/ Track
Lifecycle:
New from this manufacturer.
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