l Application Specific MOSFETs
l Ideal for CPU Core DC-DC Converters
l Low Conduction Losses
l High Cdv/dt Immunity
l Low Profile (<0.7 mm)
l Dual Sided Cooling Compatible
l Compatible with existing Surface
DSS
30V
Mount Techniques
Description
The IRF6607 combines the latest HEXFET® Power MOSFET Silicon technology with the advanced DirectFETTM packaging to
achieve the lowest on-state resistance in a package that has the footprint of an SO-8 and only 0.7 mm profile. The DirectFET
package is compatible with existing layout geometries used in power applications, PCB assembly equipment and vapor phase,
infra-red or convection soldering techniques. The DirectFET package allows dual sided cooling to maximize thermal transfer in
power systems, IMPROVING previous best thermal resistance by 80%.
The IRF6607 balances both low resistance and low charge along with ultra low package inductance to reduce both conduction
and switching losses. The reduced total losses make this product ideal for high efficiency DC-DC converters that power the
latest generation of processors operating at higher frequencies. The IRF6607 has been optimized for parameters that are
critical in synchronous buck converters including Rds(on), gate charge and Cdv/dt-induced turn on immunity. The IRF6607
offers particularly low Rds(on) and high Cdv/dt immunity for synchronous FET applications.
Absolute Maximum Ratings
ParameterUnits
V
DS
V
GS
@ TC = 25°C
I
D
@ TA = 25°C
I
D
@ TA = 70°C
I
D
I
DM
PD @TA = 25°C
PD @TA = 70°C
@TC = 25°C
P
D
T
J
T
STG
Drain-to-Source VoltageV
Gate-to-Source Voltage
Continuous Drain Current, V
Continuous Drain Current, V
Continuous Drain Current, V
Pulsed Drain Current
Power Dissipation
Power Dissipation
Power Dissipation
Linear Derating Factor W/°C
Operating Junction and°C
Storage Temperature Range
cgg
@ 10V
GS
@ 10V
GS
@ 10V
GS
-40 to + 150
3.3mΩ@V
4.4mΩ@V
Max.
30
±12
94
27
22
220
3.6
2.3
42
0.029
R
DS(on)
max
= 10V
GS
= 4.5V
GS
DirectFET ISOMETRIC
Qg
50nC
A
W
Thermal Resistance
ParameterTyp.Max.Units
R
θJA
R
θJA
R
θJA
R
θJC
R
θJ-PCB
Junct ion-to-Ambient
Junct ion-to-Ambient
Junct ion-to-Ambient
Junct ion-to-Case
Junction-to-PCB Mounted–––1.0
fgh
i
–––35
12.5–––
20–––°C/W
–––3.0
Notes through are on page 11
www.irf.com1
10/24/02
Page 2
IRF6607
/
/
gy
(
)
Static @ TJ = 25°C (unless otherwise specified)
ParameterMin. Typ. Max. Units
BV
DSS
∆Β
V
DSS
R
DS(on)
V
GS(th)
∆
V
GS(th)
I
DSS
I
GSS
gfsForward Transconductance120––––––S
Q
g
Q
gs1
Q
gs2
Q
gd
Q
godr
Q
sw
Q
oss
t
d(on)
t
r
t
d(off)
t
f
C
iss
C
oss
C
rss
Drain-to-Source Breakdown Voltage30––––––V
∆
T
Breakdown Voltage Temp. Coefficient –––29––– mV/°C
J
Static Drain-to-Source On-Resistance –––2.53.3
–––3.44.4
Gate Threshold Voltage1.0––––––V
∆
T
Gate Threshold Voltage Coefficient–––-5.3––– mV/°C
Fig 11. Maximum Effective Transient Thermal Impedance, Junction-to-Case
www.irf.com5
Page 6
IRF6607
A
15V
DRIVER
+
V
DD
-
R
V
20V
V
DS
G
GS
L
D.U.T
I
AS
Ω
0.01
t
p
Fig 12a. Unclamped Inductive Test Circuit
V
(BR)DSS
t
p
I
AS
Fig 12b. Unclamped Inductive Waveforms
120
TOP
100
80
60
40
20
AS
E , Single Pulse Avalanche Energy (mJ)
0
255075100125150
BOTTO M
Starting TJ, Junction Temperature (°C)
Fig 12c. Maximum Avalanche Energy
Vs. Drain Current
L
V
DS
D
I
D
8.9A
16A
20A
V
DD
Current Regulator
Same Type as D.U.T.
12V
.2µF
V
GS
50KΩ
3mA
.3µF
D.U.T.
V
GS
Pulse Width < 1µs
Duty Factor < 0.1%
Fig 14a. Switching Time Test Circuit
+
V
DS
-
V
DS
90%
D.U.T
10%
I
G
Current Sampling Resistors
I
D
Fig 13. Gate Charge Test Circuit
V
GS
t
d(on)tr
t
d(off)tf
Fig 14b. Switching Time Waveforms
6www.irf.com
Page 7
IRF6607
+
-
Reverse
Recovery
Current
Driver Gate Drive
P.W.
D.U.T. ISDWaveform
D.U.T. VDSWaveform
D.U.T
+
-
+
Circuit Layout Considerations
• Low Stray Inductance
• Ground Plane
-
• Low Leakage Inductance
Current Transformer
-
+
V
DD
R
G
• dv/dt controlled by R
• Driver same type as D.U.T.
• I
controlled by Duty Factor "D"
SD
• D.U.T. - Device Under Test
G
Re-Applied
Voltage
Inductor Curent
* V
GS
Period
Body Diode Forward
Current
di/dt
Diode Recovery
dv/dt
Body Diode Forward Drop
Ripple ≤ 5%
= 5V for Logic Level Devices
D =
P. W .
Period
VGS=10V
V
DD
I
SD
*
Fig 15. Peak Diode Recovery dv/dt Test Circuit for N-Channel
HEXFET® Power MOSFETs
Id
Vds
Vgs
Vgs(th)
Qgs1
Qgs2QgdQgodr
Fig 16. Gate Charge Waveform
www.irf.com7
Page 8
IRF6607
)
Power MOSFET Selection for Non-Isolated DC/DC Converters
Control FET
Special attention has been given to the power losses
in the switching elements of the circuit - Q1 and Q2.
Power losses in the high side switch Q1, also called
the Control FET, are impacted by the R
MOSFET, but these conduction losses are only about
one half of the total losses.
Power losses in the control switch Q1 are given
by;
P
= P
loss
This can be expanded and approximated by;
P
loss
conduction
= I
()
rms
+ I ×
+ Q
()
g
Q
+
This simplified loss equation includes the terms Q
and Q
charge that is included in all MOSFET data sheets.
The importance of splitting this gate-source charge
into two sub elements, Q
Fig 16.
the gate driver between the time that the threshold
voltage has been reached and the time the drain current rises to I
gins to change. Minimizing Q
reducing switching losses in Q1.
put capacitance of the MOSFET during every switching cycle. Figure A shows how Q
parallel combination of the voltage dependant (nonlinear) capacitances Cds and Cdg when multiplied by
the power supply input buss voltage.
which are new to Power MOSFET data sheets.
oss
Q
is a sub element of traditional gate-source
gs2
Q
indicates the charge that must be supplied by
gs2
Q
is the charge that must be supplied to the out-
oss
2
Q
× R
gd
i
g
+ P
ds(on )
× Vin× f
switching
+ P
+ I ×
drive
Q
+ P
gs 2
i
g
× Vg× f
oss
2
dmax
×Vin× f
and Q
gs1
at which time the drain voltage be-
, can be seen from
gs2
is a critical factor in
gs2
is formed by the
oss
of the
ds(on)
output
× Vin× f
Synchronous FET
The power loss equation for Q2 is approximated
by;
P
= P
loss
P
loss
+ Qg× Vg× f
+
conduction
= I
rms
()
Q
*dissipated primarily in Q1.
For the synchronous MOSFET Q2, R
portant characteristic; however, once again the im-
portance of gate charge must not be overlooked since
it impacts three critical areas. Under light load the
MOSFET must still be turned on and off by the control IC so the gate drive losses become much more
significant. Secondly, the output charge Q
verse recovery charge Qrr both generate losses that
are transfered to Q1 and increase the dissipation in
that device. Thirdly, gate charge will impact the
MOSFETs’ susceptibility to Cdv/dt turn on.
gs2
The drain of Q2 is connected to the switching node
of the converter and therefore sees transitions between ground and Vin. As Q1 turns on and off there is
a rate of change of drain voltage dV/dt which is capacitively coupled to the gate of Q2 and can induce
a voltage spike on the gate that is sufficient to turn
the MOSFET on, resulting in shoot-through current .
The ratio of Qgd/Q
potential for Cdv/dt turn on.
Figure A: Q
+ P
2
× R
ds(on)()
oss
×Vin× f
2
must be minimized to reduce the
gs1
Characteristic
oss
drive
*
+ P
output
+ Qrr× Vin× f
(
ds(on)
oss
is an im-
and re-
8www.irf.com
Page 9
DirectFET Outline Dimension
IRF6607
www.irf.com9
Page 10
IRF6607
DirectFET PCB Footprint
DirectFET
10www.irf.com
Tape and Reel Dimension
Page 11
DirectFET Part Marking
IRF6607
Notes:
Repetitive rating; pulse width limited by
max. junction temperature.
Starting T
RG = 25Ω, I
Pulse width ≤ 400µs; duty cycle ≤ 2%.
IR WORLD HEADQUARTERS: 233 Kansas St., El Segundo, California 90245, USA Tel: (310) 252-7105
= 25°C, L = 0.25mH
J
= 20A.
AS
This product has been designed and qualified for the Consumer market.
Surface mounted on 1 in. square Cu board.
Used double sided cooling , mounting pad.
Mounted on minimum footprint full size board with metalized
back and with small clip heatsink.
T
measured with thermal couple mounted to top (Drain) of
C
part.
Data and specifications subject to change without notice.
Qualification Standards can be found on IR’s Web site.
TAC Fax: (310) 252-7903
Visit us at www.irf.com for sales contact information.10/02
www.irf.com11
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