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ISL6612_14 Datasheet, PDF (9/12 Pages) Intersil Corporation – Advanced Synchronous Rectified Buck MOSFET Drivers with Protection Features
ISL6612, ISL6613
is approximately 800mW at room temperature, while the
power dissipation capacity in the EPSOIC and DFN
packages, with an exposed heat escape pad, is more than 2W
and 1.5W, respectively. Both EPSOIC and DFN packages are
more suitable for high frequency applications. See “Layout
Considerations” on page 9 for thermal transfer improvement
suggestions. When designing the driver into an application, it
is recommended that the following calculation is used to
ensure safe operation at the desired frequency for the
selected MOSFETs. The total gate drive power losses due to
the gate charge of MOSFETs and the driver’s internal circuitry
and their corresponding average driver current can be
estimated using Equation 2 and Equation 3, respectively,
PQg_TOT = PQg_Q1 + PQg_Q2 + IQ • VCC
P Q g _Q1
=
Q-----G-----1----•-----U----V-----C-----C----2--
VGS1
•
FS
W
•
NQ
1
PQ g _Q2
=
Q-----G-----2----•-----L---V-----C-----C----2--
VGS2
•
FSW
•
NQ2
(EQ. 2)
IDR
=
⎛
⎜
⎝
Q-----G-----1----•-----U----V-----C-----C-----•-----N----Q-----1-
VGS1
+
-Q----G-----2----•-----LV---V--G---C-S----C2-----•-----N----Q-----2-⎠⎟⎞
• FSW + IQ
(EQ. 3)
where the gate charge (QG1 and QG2) is defined at a
particular gate to source voltage (VGS1and VGS2) in the
corresponding MOSFET data sheet; IQ is the driver’s total
quiescent current with no load at both drive outputs; NQ1
and NQ2 are number of upper and lower MOSFETs,
respectively; UVCC and LVCC are the drive voltages for
both upper and lower FETs, respectively. The IQ*VCC
product is the quiescent power of the driver without
capacitive load and is typically 116mW at 300kHz.
The total gate drive power losses are dissipated among the
resistive components along the transition path. The drive
resistance dissipates a portion of the total gate drive power
losses, the rest will be dissipated by the external gate
resistors (RG1 and RG2) and the internal gate resistors (RGI1
and RGI2) of MOSFETs. Figures 3 and 4 show the typical
upper and lower gate drives turn-on transition path. The
power dissipation on the driver can be roughly estimated as:
PDR = PDR_UP + PDR_LOW + IQ • VCC
P D R _UP
=
⎛
⎜
⎝
-------------R-----H----I--1--------------
RHI1 + REXT1
+
R-----L---O-----1R----+-L---O-R----1-E----X----T---1- ⎠⎟⎞
•
P-----Q----g----_---Q----1-
2
P D R _LOW
=
⎛
⎜
⎝
-------------R-----H----I--2--------------
RHI2 + REXT2
+
-R----L---O-----2R----+-L---O-R----2-E----X----T---2- ⎠⎟⎞
•
P-----Q----g----_--Q-----2-
2
REXT1
=
RG1
+
R-----G-----I-1--
NQ1
REXT2
=
RG2
+
R-----G-----I-2--
NQ2
(EQ. 4)
UVCC
BOOT
D
RHI1
RLO1
PHASE
CGD
G
RG1
RGI1
CGS
S
CDS
Q1
FIGURE 3. TYPICAL UPPER-GATE DRIVE TURN-ON PATH
LVCC
RHI2
RLO2
CGD
G
RG2
RGI2
CGS
S
D
CDS
Q2
FIGURE 4. TYPICAL LOWER-GATE DRIVE TURN-ON PATH
Layout Considerations
For heat spreading, place copper underneath the IC whether
it has an exposed pad or not. The copper area can be
extended beyond the bottom area of the IC and/or
connected to buried copper plane(s) with thermal vias. This
combination of vias for vertical heat escape, extended
copper plane, and buried planes for heat spreading allows
the IC to achieve its full thermal potential.
Place each channel power component as close to each
other as possible to reduce PCB copper losses and PCB
parasitics: shortest distance between DRAINs of upper FETs
and SOURCEs of lower FETs; shortest distance between
DRAINs of lower FETs and the power ground. Thus, smaller
amplitudes of positive and negative ringing are on the
switching edges of the PHASE node. However, some space
in between the power components is required for good
airflow. The traces from the drivers to the FETs should be
kept short and wide to reduce the inductance of the traces
and to promote clean drive signals.
9
FN9153.9
June 15, 2010