LTC3605
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ESR is the effective series resistance of C
OUT
. DI
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 problem.
The initial output voltage step may not be within the band
-
width of the feedback loop, so the standard second order
overshoot/
DC ratio cannot be used to determine phase
margin. The gain of the loop increases with the R and the
bandwidth of the loop increases with decreasing C. If R
is increased by the same factor that C is decreased, the
zero frequency will be kept the same, thereby keeping the
phase the same in the most critical frequency range of the
feedback loop. In addition, a feedforward capacitor, C
FF
,
can be added to improve the high frequency response, as
shown in Figure 1. Capacitor C
FF
provides phase lead by
creating a high frequency zero with R2 which improves
the phase margin.
The output voltage settling behavior is related to the stability
of the closed-loop system and will demonstrate the actual
overall supply performance. For a detailed explanation of
optimizing the compensation components, including a
review of control loop theory, refer to Linear Technology
Application Note 76.
In some applications, a more severe transient can be caused
by switching in loads with large (>10µF) input capacitors.
The discharged input capacitors are effectively put in paral
-
lel with C
OUT
, causing a rapid drop in V
OUT
. No regulator
can deliver enough current to prevent this problem, if
the switch connecting the load has low resistance and is
driven quickly. The solution is to limit the turn-on speed of
the load switch driver. A Hot Swap controller is designed
specifically for this purpose and usually incorporates
current limiting, short-circuit protection and soft-starting.
Efficiency Considerations
The percent 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
operaTion
Table 1. Inductor Selection Table
INDUCTANCE DCR MAX CURRENT DIMENSIONS HEIGHT
Vishay IHLP-2525CZ-01 Series
0.33µH 4.1mW 18A 6.7mm × 7mm 3mm
0.47µH 6.5mW 13.5A
0.68µH 9.4mW 11A
0.82µH 11.8mW 10A
1.0µH 14.2mW 9A
Vishay IHLP-1616BZ-11 Series
0.22µH 4.1mW 12A 4.3mm × 4.7mm 2.0mm
0.47µH 15mW 7A
Toko FDV0620 Series
0.20µH 4.5mW 12.4A 7mm × 7.7mm 2.0mm
0.47µH 8.3mW 9A
1µH 18.3mW 5.7A
NEC/Tokin MLC0730L Series
0.47µH 4.5mW 16.6A 6.9mm × 7.7mm 3.0mm
0.75µH 7.5mW 12.2A
1µH 9mW 10.6A
Cooper HCP0703 Series
0.22µH 2.8mW 23A 7mm × 7.3mm 3.0mm
0.47µH 4.2mW 17A
0.68µH 5.5mW 15A
0.82µH 8mW 13A
1µH 10mW 11A
1.5µH 14mW 9A
TDK RLF7030 Series
1µH 8.8mW 6.4A 6.9mm × 7.3mm 3.2mm
1.5µH 9.6mW 6.1A
2.2µH 12mW 5.4A
Würth Elektronik WE-HC 744312 Series
0.25µH 2.5mW 18A 7mm × 7.7mm 3.8mm
0.47µH 3.4mW 16A
0.72µH 7.5mW 12A
1µH 9.5mW 11A
1.5µH 10.5mW 9A
LTC3605
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For more information www.linear.com/LTC3605
operaTion
produce the most improvement. Percent efficiency can
be expressed as:
% Efficiency = 100%–(L1 + L2 + L3 +…)
where L1, L2, etc. are the individual losses as a percent
-
age of input power.
Although all
dissipative elements in the circuit produce
losses, three main sources usually account for most of
the losses in LTC3605 circuits: 1) I
2
R losses, 2) switching
and biasing losses, 3) other losses.
1. I
2
R losses are calculated from the DC resistances of
the internal switches, R
SW
, and external inductor, R
L
.
In continuous mode, the average output current flows
through inductor L but is chopped between the
internal top and bottom power MOSFETs. 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)
The R
DS(ON)
for both the top and bottom MOSFETs can be
obtained from the Typical Performance Characteristics
curves. Thus to obtain I
2
R losses:
I
2
R losses = I
OUT
2
(R
SW
+ R
L
)
2. The INTV
CC
current is the sum of the power MOSFET
driver and control currents. The power MOSFET driver
current results from switching the gate capacitance of
the power MOSFETs. Each time a power MOSFET gate is
switched from low to high to low again, a packet of charge
dQ moves from INTV
CC
to ground. The resulting dQ/dt
is a current out of INTV
CC
that is typically much larger
than the DC control 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 power MOSFETs
and f is the switching frequency. Since INTV
CC
is a low
dropout regulator output powered by V
IN
, its power
loss equals:
P
LDO
= V
IN
I
INTVCC
Refer to the I
INTVCC
vs Frequency curve in the Typical
Performance Characteristics for typical INTV
CC
current
at various frequencies.
3. Other “hidden” losses such as transition loss and cop
-
per trace and internal load resistances can account for
additional efficiency
degradations in the overall power
system. It is very important to include these “system”
level losses in the design of a system. Transition loss
arises from the brief amount of time the top power
MOSFET spends in the saturated region during switch
node transitions. The LTC3605 internal power devices
switch quickly enough that these losses are not signifi
-
cant compared to other sources. Other losses including
diode conduction losses during dead-time and inductor
core losses which generally account for less than
2%
total additional loss.
Thermal Considerations
In a majority of applications
, the LTC3605 does not dis
-
sipate much heat due to its high efficiency and low thermal
resistance of its exposed-back QFN package. However, in
applications where the LTC3605 is running at high ambi
-
ent temperature, high V
IN
, high switching frequency and
maximum output current load, the heat dissipated may
exceed the maximum junction temperature of the part.
If the junction temperature reaches approximately 160°C,
both power switches will be turned off until the temperature
drops about 15°C cooler.
To avoid the LTC3605 from exceeding the maximum junc
-
tion 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 temperature rise is
given by:
T
RISE
= P
D
θ
JA
As an example, consider the case when the LTC3605 is used
in applications where V
IN
= 12V, I
OUT
= 5A, f = 1MHz, V
OUT
= 1.8V. The equivalent power MOSFET resistance R
SW
is:
R
SW
= R
DS(ON)
Top
V
OUT
V
IN
+R
DS(ON)
Bot 1
V
OUT
V
IN
= 70mW
1.8
12
+ 35mW
10.2
12
= 40.25mW
LTC3605
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For more information www.linear.com/LTC3605
operaTion
The V
IN
current during 1MHz force continuous operation
with no load is about 11mA, which includes switching
and internal biasing current loss, transition loss, inductor
core loss and other losses in the application. Therefore,
the total power dissipated by the part is:
P
D
= I
OUT
2
R
SW
+ V
IN
I
VIN
(No Load)
= 25A
2
40.25mΩ + 12V 11mA = 1.14W
The QFN 4mm × 4mm package junction-to-ambient thermal
resistance, θ
JA
, is around 37°C/W. Therefore, the junction
temperature of the regulator operating in a 25°C ambient
temperature is approximately:
T
J
= 1.14W 37°C/W + 25°C = 67°C
Remembering that the above junction temperature is
obtained from an R
DS(ON)
at 25°C, we might recalculate
the junction temperature based on a higher R
DS(ON)
since
it increases with temperature. Redoing the calculation
assuming that R
SW
increased 15% at 67°C yields a new
junction temperature of 72°C. If the application calls for
a higher ambient temperature and/or higher switching
frequency, care should be taken to reduce the temperature
rise of the part by using a heat sink or air flow. Figure 2
is a temperature derating curve based on the DC1215
demo board.
Junction Temperature Measurement
The junction-to-ambient thermal resistance will vary de-
pending on the size and amount of heat sinking copper
on the PCB board where the part is mounted,
as well as
the amount of air flow on the device. One of the ways to
measure the junction temperature directly is to use the
internal junction diode on one of the pins (PGOOD) to
measure its diode voltage change based on ambient
temperature change. First remove any external passive
component on the PGOOD pin, then pull out 100µA from
the PGOOD pin to turn on its internal junction diode and
bias the PGOOD pin to a negative voltage. With no output
current load, measure the PGOOD voltage at an ambient
temperature of 25°C, 75°C and 125°C to establish a slope
relationship between the delta voltage on PGOOD and
delta ambient temperature. Once this slope is established,
then the junction temperature rise can be measured as a
function of power loss in the package with corresponding
output load current. Keep in mind that doing so will violate
absolute maximum voltage ratings on the PGOOD pin,
however, with the limited current, no damage will result.
Board Layout Considerations
When laying out the printed circuit board, the following
checklist should be used to ensure proper operation of
the LTC3605 (refer to Figure 3). Check the following in
your layout:
1. Do the capacitors C
IN
connect to the power PV
IN
and
power PGND as close as possible? These capacitors
provide the AC current to the internal power MOSFETs
and their drivers.
2. Are C
OUT
and L1 closely connected? The (–) plate of
C
OUT
returns current to PGND and the (–) plate of C
IN
.
3. The resistive divider, R1 and R2, must be connected
between the (+) plate of C
OUT
and a ground line termi-
nated near SGND. The feedback signal V
FB
should be
routed away from noisy components and traces, such
as the SW line, and its trace should be minimized. Keep
R1 and R2 close to the IC.
AMBIENT TEMPERATURE (°C)
20
0
LOAD CURRENT (A)
1
2
3
4
6
40
60 80 100
3605 F02
120 140
5
V
IN
= 12V
V
OUT
= 3.3V
f
SW
= 1MHz
DC1215 DEMO BOARD
Figure 2. Load Current vs Ambient Temperature

LTC3605EUF#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 14V, 5A PolyPhase Synchronous Step Down Regulator
Lifecycle:
New from this manufacturer.
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