English
Language : 

LTC3730_15 Datasheet, PDF (14/28 Pages) Linear Technology – 3-Phase, 5-Bit Intel Mobile VID, 600kHz, Synchronous Buck Controller
LTC3730
APPLICATIO S I FOR ATIO
drain-to-gate accumulation capacitance and the gate-to-
source capacitance. The Miller charge (the increase in
coulombs on the horizontal axis from a to b while the curve
is flat) is specified for a given VDS drain voltage, but can be
adjusted for different VDS voltages by multiplying by the
ratio of the application VDS to the curve specified VDS
values. A way to estimate the CMILLER term is to take the
change in gate charge from points a and b on a manufac-
turers data sheet and divide by the stated VDS voltage
specified. CMILLER is the most important selection criteria
for determining the transition loss term in the top MOSFET
but is not directly specified on MOSFET data sheets. CRSS
and COS are specified sometimes but definitions of these
parameters are not included.
MILLER EFFECT
VGS
V
a
b
QIN
+
CMILLER = (QB – QA)/VDS
VGS
–
Figure 5
VIN
+
VDS
–
3730 F05
When the controller is operating in continuous mode the
duty cycles for the top and bottom MOSFETs are given by:
Main Switch Duty Cycle = VOUT
VIN
Synchronous
Switch Duty
Cycle
=
⎛
⎝⎜
VIN
– VOUT
VIN
⎞
⎠⎟
The power dissipation for the main and synchronous
MOSFETs at maximum output current are given by:
( ) PMAIN
=
VOUT
VIN
⎛ IMAX ⎞ 2
⎝⎜ N ⎠⎟
1+ δ
RDS(ON)
+
( )( ) VIN2
IMAX
2N
RDR
C MILLER
•
( ) ⎡
⎢
1
+
1
⎤
⎥f
⎣⎢VCC – VTH(IL) VTH(IL) ⎦⎥
( ) PSYNC
=
VIN
– VOUT
VIN
⎛ IMAX ⎞ 2
⎝⎜ N ⎠⎟
1+ δ
RDS(ON)
14
where N is the number of output stages, δ is the tempera-
ture dependency of RDS(ON), RDR is the effective top driver
resistance (approximately 2Ω at VGS = VMILLER), VIN is the
drain potential and the change in drain potential in the
particular application. VTH(IL) is the data sheet specified
typical gate threshold voltage specified in the power
MOSFET data sheet at the specified drain current. CMILLER
is the calculated capacitance using the gate charge curve
from the MOSFET data sheet and the technique described
above.
Both MOSFETs have I2R losses while the topside N-channel
equation includes an additional term for transition losses,
which peak at the highest input voltage. For VIN < 12V, the
high current efficiency generally improves with larger
MOSFETs, while for VIN > 12V, the transition losses
rapidly increase to the point that the use of a higher
RDS(ON) device with lower CMILLER actually provides higher
efficiency. The synchronous MOSFET losses are greatest
at high input voltage when the top switch duty factor is low
or during a short circuit when the synchronous switch is
on close to 100% of the period.
The term (1 + δ ) is generally given for a MOSFET in the
form of a normalized RDS(ON) vs temperature curve, but
δ = 0.005/°C can be used as an approximation for low
voltage MOSFETs.
The Schottky diodes, (D1 to D3 in Figure 1) conduct during
the dead time between the conduction of the two large
power MOSFETs. This prevents the body diode of the
bottom MOSFET from turning on, storing charge during
the dead time and requiring a reverse recovery period
which could cost as much as several percent in efficiency.
A 2A to 8A Schottky is generally a good compromise for
both regions of operation due to the relatively small
average current. Larger diodes result in additional transi-
tion loss due to their larger junction capacitance.
CIN and COUT Selection
In continuous mode, the source current of each top
N-channel MOSFET is a square wave of duty cycle VOUT/VIN.
A low ESR input capacitor sized for the maximum RMS
current must be used. The details of a close form equation
can be found in Application Note 77. Figure 6 shows the
input capacitor ripple current for different phase configu-
3730fa