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The peak inductor current when operating in the buck
region is:
I
L(MAX,BUCK)
I
OUT(MAX)
+
V
OUT(MIN)
DC
(MAX,M2,BUCK
100%
2L f
A
where DC
(MAX,M2,BUCK)
is the maximum duty cycle percent-
age of the M2 switch in the buck region given by:
DC
MAX,M2,BUCK
( )
1–
V
OUT(MIN)
V
IN(MAX)
100%
Note that the inductor current can be higher during load
transients and if the load current exceeds the expected
maximum I
OUT(MAX)
. It can also be higher during start-
up if inadequate soft-start capacitance is used or during
output shorts. Consider using the output current limiting
to prevent the inductor current from becoming excessive.
Output current limiting is discussed later in the Input/
Output Current Monitoring and Limiting section. Care
-
ful board evaluation of the maximum inductor current
is recommended.
Power MOSFET Selection and Efficiency
Considerations
The LT8705 requires four external N-channel power MOS
-
FETs, two for the top switches (switches M1 and M4, shown
in Figure 3) and two for the bottom switches (switches
M2 and M3, shown in Figure 3). Important parameters for
the power MOSFETs are the breakdown voltage, V
BR,DSS
,
threshold voltage, V
GS,TH
, on-resistance, R
DS(ON)
, reverse-
transfer capacitance, C
RSS
(gate-to-drain capacitance), and
maximum current, I
DS(MAX)
. The gate drive voltage is set
by the 6.35V GATEV
CC
supply. Consequently, logic-level
threshold MOSFETs must be used in LT8705 applications.
It is very important to consider power dissipation when
selecting power MOSFETs. The most
efficient circuit will
use MOSFETs that dissipate the least amount of power.
Power dissipation must be limited to avoid overheating
that might damage the devices. For most buck-boost ap
-
plications the
M1 and M3 switches will have the highest
power dissipation where M2 will have the lowest unless
the output becomes shorted. In some cases it can be
helpful to use two or more MOSFETs in parallel to reduce
power dissipation in each device. This is most helpful when
power is dominated by I
2
R losses while the MOSFET is
“on”. The additional capacitance of connecting MOSFETs
in parallel can sometimes slow down switching edge rates
and consequently increase total switching power losses.
The following sections provide guidelines for calculating
power consumption of the individual MOSFETs. From a
known power dissipation, the MOSFET junction tempera
-
ture can be obtained using the following formula:
T
J
= T
A
+ PR
TH(JA)
where:
T
J
is the junction temperature of the MOSFET
T
A
is the ambient air temperature
P is the power dissipated in the MOSFET
R
TH(JA)
is the MOSFET’s thermal resistance from the
junction to the ambient air. Refer to the manufacturer’s
data sheet.
R
TH(JA)
normally includes the R
TH(JC)
for the device plus
the thermal resistance from the case to the ambient tem-
perature R
TH(JC)
. Compare the calculated value of T
J
to
the manufacturer’s data sheets to help choose MOSFETs
that will not overheat.
Switch M1: The power dissipation in switch M1 comes
from two primary components: (1) I
2
R power when the
switch is fully turnedon” and inductor current is flowing
through the drain to source connections and (2) power
dissipated while the switch is turningon” oroff”. As the
switch turnson” andoff” a combination of high current
and high voltage causes high power dissipation in the
MOSFET. Although the switching times are short, the aver
-
age power dissipation can still be significant and is often
the
dominant source of power in the MOSFET. Depending
on the application, the maximum power dissipation in
the M1 switch can happen in the buck region when V
IN
is highest, V
OUT
is highest, and switching power losses
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are greatest or in the boost region when V
IN
is smallest,
V
OUT
is highest and M1 is always on. Switch M1 power
consumption can be approximated as:
P
M1
=P
I
2
R
+P
SWITCHING
V
OUT
V
IN
I
OUT
2
R
DS(ON)
ρ
τ
+ V
IN
I
OUT
f t
RF1
( )
W BUCK REGION
( )
V
OUT
V
IN
I
OUT
2
R
DS(ON)
ρ
τ
+ 0W (BOOST REGION)
where:
the P
SWITCHING
term is 0 in the boost region
t
RF1
is the average of the SW1 pin rise and fall times.
Typical values are 20ns to 40ns depending on the
MOSFET capacitance and V
IN
voltage.
ρ
τ
is a normalization factor (unity at 25°C) accounting
for the significant variation in MOSFET on-resistance
with temperature, typically about 0.4%/°C, as shown
in Figure 9. For a maximum junction temperature of
125°C, using a value ρ
τ
= 1.5 is reasonable.
JUNCTION TEMPERATURE (°C)
–50
ρ
τ
NORMALIZED ON-RESISTANCE (Ω)
1.0
1.5
150
8705 F09
0.5
0
0
50
100
2.0
Figure 9. Normalized MOSFET R
DS(ON)
vs Temperature
Since the switching power (P
SWITCHING
) often dominates,
look for MOSFETs with lower C
RSS
or consider operating
at a lower frequency to minimize power loss and increase
efficiency.
Switch M2: In most cases the switching power dissipa
-
tion in the M2 switch is quite small and I
2
R power losses
dominate. I
2
R power is greatest in the buck region where
the switch operates as the synchronous rectifier. Higher
V
IN
and lower V
OUT
causes the M2 switch to beon” for
the most amount of time, leading to the highest power
consumption. The M2 switch power consumption in the
buck region can be approximated as:
P
(M2,BUCK)
V
IN
V
OUT
V
IN
I
OUT(MAX)
2
R
DS(ON)
ρ
τ
W
Switch M3: Switch M3 operates in the boost and buck-boost
regions as a control switch. Similar to the M1 switch, the
power dissipation comes from I
2
R power and switching
power. The maximum power dissipation is when V
IN
is
the lowest and V
OUT
is the highest. The following expres-
sion approximates
the power dissipation in the M3 switch
under those conditions:
P
M3
=P
I
2
R
+P
SWITCHING
V
OUT
V
IN
( )
V
OUT
V
IN
2
I
OUT
2
R
DS(ON)
ρ
τ
+ V
OUT
2
I
OUT
f
t
RF2
V
IN
W
where the total power is 0 in the buck region.
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t
RF2
is the average of the SW2 pin rise and fall times and,
similar to t
RF1
, is typically 20ns to 40ns.
As with the M1 switch, the switching power (P
SWITCHING
)
often dominates. Look for MOSFETs with lower C
RSS
or
consider operating at a lower frequency to minimize power
loss and increase efficiency.
Switch M4: In most cases the switching power dissipa
-
tion in the M4 switch is quite small and I
2
R power losses
dominate. I
2
R power is greatest in the boost region where
the switch operates as the synchronous rectifier. Lower
V
IN
and higher V
OUT
increases the inductor current for a
given I
OUT
, leading to the highest power consumption.
The M4 switch power consumption in the boost region
can be approximated as:
P
(M4,BOOST)
V
OUT
V
IN
I
OUT
2
ρ
τ
R
DS(ON)
W
Gate Resistors: In some cases it can be beneficial to add
to 10Ω of resistance between some of the NMOS gate
pins and their respective gate driver pins on the LT8705
(i.e., TG1, BG1, TG2, BG2). Due to parasitic inductance
and capacitance, ringing can occur on SW1 or SW2 when
low capacitance MOSFETs are turned on/off too quickly.
The ringing can be of greatest concern when operating
the MOSFETs or the LT8705 near the rated voltage limits.
Additional gate resistance slows the switching speed,
minimizing the ringing.
Excessive gate resistance can have two negative side ef-
fects on performance:
1.
Slowing the switch transition times can also increase
power dissipation in the switch. This is described above
in the Switch M1 and Switch M3 sections.
2. Capacitive coupling from the SW1 or SW2 pin to the
switch gate node can turn it on when it’s supposed to be
off, thus increasing power dissipation. With too much
gate resistance, this would most commonly happen to
the M2 switch when SW1 is rising.
Careful board evaluation should be performed when
optimizing the gate resistance values. SW1 and SW2 pin
ringing can be affected by the inductor current levels,
therefore board evaluation should include measurements
at a wide range of load currents. When performing PCB
measurements of the SW1 and SW2 pins, be sure to use a
very short ground post from the PCB ground to the scope
probe ground sleeve in order to minimize false inductive
voltages readings.
C
IN
and C
OUT
Selection
Input and output capacitance is necessary to suppress
voltage ripple caused by discontinuous current moving in
and out of the regulator. A parallel combination of capaci
-
tors is typically used to achieve high capacitance and low
ESR
(equivalent series resistance). Dry tantalum, special
polymer, aluminum electrolytic and ceramic capacitors are
all available in surface mount packages. Capacitors with
low ESR and high ripple current ratings, such as OS-CON
and POSCAP are also available.
Ceramic capacitors should be placed near the regulator
input and output to suppress high frequency switching
spikes. A ceramic capacitor, of at leastF, should also
be placed from V
IN
to GND as close to the LT8705 pins
as possible. Due to their excellent low ESR characteristics
ceramic capacitors can significantly reduce input ripple
voltage and help reduce power
loss in the higher ESR bulk
capacitors. X5R or X7R dielectrics are preferred, as these
materials retain their capacitance over wide voltage and
temperature ranges. Many ceramic capacitors, particularly
0805 or 0603 case sizes, have greatly reduced capacitance
at the desired operating voltage.
Input Capacitance: Discontinuous input current is highest
in the buck region due to the M1 switch toggling on and off.
Make sure that the C
IN
capacitor network has low enough
ESR and is sized to handle the maximum RMS current.
For buck operation, the input RMS current is given by:
I
RMS
I
OUT(MAX)
V
OUT
V
IN
V
IN
V
OUT
1
This formula has a maximum at V
IN
= 2V
OUT
, where
I
RMS
= I
OUT(MAX)
/2. This simple worst-case condition
is commonly used for design because even significant
deviations do not offer much relief.

LT8705MPFE#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 80V Vin and Vout Synchronous 4-Switch Buck- Boost DC/DC Controller
Lifecycle:
New from this manufacturer.
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