1
Motorola TMOS Power MOSFET Transistor Device Data
Designer's
TM
Data Sheet
Medium Power Surface Mount Products
TMOS Single P-Channel
Field Effect Transistors
MiniMOS
TM
devices are an advanced series of power MOSFETs
which utilize Motorola's High Cell Density HDTMOS process.
These miniature surface mount MOSFETs feature ultra low RDS(on)
and true logic level performance. They are capable of withstanding
high energy in the avalanche and commutation modes and the
draintosource diode has a very low reverse recovery time.
MiniMOS devices are designed for use in low voltage, high speed
switching applications where power efficiency is important. Typical
applications are dcdc converters, and power management in
portable and battery powered products such as computers,
printers, cellular and cordless phones. They can also be used for
low voltage motor controls in mass storage products such as disk
drives and tape drives. The avalanche energy is specified to
eliminate the guesswork in designs where inductive loads are
switched and offer additional safety margin against unexpected
voltage transients.
·
Ultra Low RDS(on) Provides Higher Efficiency and Extends Battery Life
·
Logic Level Gate Drive -- Can Be Driven by Logic ICs
·
Miniature SO8 Surface Mount Package -- Saves Board Space
·
Diode Is Characterized for Use In Bridge Circuits
·
Diode Exhibits High Speed, With Soft Recovery
·
IDSS Specified at Elevated Temperature
·
Avalanche Energy Specified
·
Mounting Information for SO8 Package Provided
MAXIMUM RATINGS
(TJ = 25
°
C unless otherwise noted)(1)
Rating
Symbol
Value
Unit
DraintoSource Voltage
VDSS
20
Vdc
DraintoGate Voltage (RGS = 1.0 M
)
VDGR
20
Vdc
GatetoSource Voltage -- Continuous
VGS
±
20
Vdc
Drain Current -- Continuous @ TA = 25
°
C
Drain Current
-- Continuous @ TA = 100
°
C
Drain Current
-- Single Pulse (tp
10
µ
s)
ID
ID
IDM
5.6
3.6
30
Adc
Apk
Total Power Dissipation @ TA = 25
°
C (2)
PD
2.5
Watts
Operating and Storage Temperature Range
TJ, Tstg
55 to 150
°
C
Single Pulse DraintoSource Avalanche Energy -- Starting TJ = 25
°
C
(VDD = 20 Vdc, VGS = 5.0 Vdc, Peak IL = 9.0 Apk, L = 14
mH, RG = 25
)
EAS
567
mJ
Thermal Resistance -- Junction to Ambient (2)
R
JA
50
°
C/W
Maximum Lead Temperature for Soldering Purposes, 1/8
from case for 10 seconds
TL
260
°
C
DEVICE MARKING
S3P02
(1) Negative sign for PChannel device omitted for clarity.
(2) Mounted on 2" square FR4 board (1" sq. 2 oz. Cu 0.06" thick single sided), 10 sec. max.
ORDERING INFORMATION
Device
Reel Size
Tape Width
Quantity
MMSF3P02HDR2
13
12 mm embossed tape
2500 units
Designer's Data for "Worst Case" Conditions -- The Designer's Data Sheet permits the design of most circuits entirely from the information presented. SOA Limit
curves -- representing boundaries on device characteristics -- are given to facilitate "worst case" design.
Designer's, HDTMOS and MiniMOS are trademarks of Motorola, Inc. TMOS is a registered trademark of Motorola, Inc.
Thermal Clad is a trademark of the Bergquist Company.
Order this document
by MMSF3P02HD/D
MOTOROLA
SEMICONDUCTOR TECHNICAL DATA
©
Motorola, Inc. 1996
CASE 75105, Style 13
SO8
NC
1
2
3
4
8
7
6
5
Top View
Source
Source
Gate
Drain
Drain
Drain
Drain
D
S
G
MMSF3P02HD
SINGLE TMOS
POWER MOSFET
3.0 AMPERES
20 VOLTS
RDS(on) = 0.075 OHM
Motorola Preferred Device
TM
Preferred devices are Motorola recommended choices for future use and best overall value.
REV 5
MMSF3P02HD
2
Motorola TMOS Power MOSFET Transistor Device Data
ELECTRICAL CHARACTERISTICS
(TA = 25
°
C unless otherwise noted)(1)
Characteristic
Symbol
Min
Typ
Max
Unit
OFF CHARACTERISTICS
DraintoSource Breakdown Voltage
(VGS = 0 Vdc, ID = 250
µ
Adc)
Temperature Coefficient (Positive)
V(BR)DSS
20
--
--
24
--
--
Vdc
mV/
°
C
Zero Gate Voltage Drain Current
(VDS = 20 Vdc, VGS = 0 Vdc)
(VDS = 20 Vdc, VGS = 0 Vdc, TJ = 125
°
C)
IDSS
--
--
--
--
1.0
10
µ
Adc
GateBody Leakage Current (VGS =
±
20 Vdc, VDS = 0)
IGSS
--
--
100
nAdc
ON CHARACTERISTICS(2)
Gate Threshold Voltage
(VDS = VGS, ID = 250
µ
Adc)
Temperature Coefficient (Negative)
VGS(th)
1.0
--
1.5
4.0
2.0
--
Vdc
mV/
°
C
Static DrainSource OnResistance
(VGS = 10 Vdc, ID = 3.0 Adc)
(VGS = 4.5 Vdc, ID = 1.5 Adc)
RDS(on)
--
--
0.06
0.08
0.075
0.095
Ohm
Forward Transconductance (VDS = 3.0 Vdc, ID = 1.5 Adc)
gFS
3.0
7.2
--
mhos
DYNAMIC CHARACTERISTICS
Input Capacitance
(VDS = 16 Vdc, VGS = 0 Vdc,
f = 1.0 MHz)
Ciss
--
1010
1400
pF
Output Capacitance
(VDS = 16 Vdc, VGS = 0 Vdc,
f = 1.0 MHz)
Coss
--
740
920
Transfer Capacitance
f = 1.0 MHz)
Crss
--
260
490
SWITCHING CHARACTERISTICS(3)
TurnOn Delay Time
(VDD = 10 Vdc, ID = 3.0 Adc,
VGS = 4.5 Vdc,
RG = 6.0
)
td(on)
--
25
50
ns
Rise Time
(VDD = 10 Vdc, ID = 3.0 Adc,
VGS = 4.5 Vdc,
RG = 6.0
)
tr
--
135
270
TurnOff Delay Time
VGS = 4.5 Vdc,
RG = 6.0
)
td(off)
--
54
108
Fall Time
G = 6.0
)
tf
--
84
168
TurnOn Delay Time
(VDD = 10 Vdc, ID = 3.0 Adc,
VGS = 10 Vdc,
RG = 6.0
)
td(on)
--
16
32
Rise Time
(VDD = 10 Vdc, ID = 3.0 Adc,
VGS = 10 Vdc,
RG = 6.0
)
tr
--
40
80
TurnOff Delay Time
VGS = 10 Vdc,
RG = 6.0
)
td(off)
--
110
220
Fall Time
G = 6.0
)
tf
--
97
194
Gate Charge
See Figure 8
(VDS = 16 Vdc, ID = 3.0 Adc,
VGS = 10 Vdc)
QT
--
33
46
nC
See Figure 8
(VDS = 16 Vdc, ID = 3.0 Adc,
VGS = 10 Vdc)
Q1
--
3.0
--
(VDS = 16 Vdc, ID = 3.0 Adc,
VGS = 10 Vdc)
Q2
--
11
--
Q3
--
10
--
SOURCEDRAIN DIODE CHARACTERISTICS
Forward OnVoltage(2)
(IS = 3.0 Adc, VGS = 0 Vdc)
(IS = 3.0 Adc, VGS = 0 Vdc, TJ = 125
°
C)
VSD
--
--
1.35
0.96
1.75
--
Vdc
Reverse Recovery Time
See Figure 15
(IS = 3.0 Adc, VGS = 0 Vdc,
dIS/dt = 100 A/
µ
s)
trr
--
76
--
ns
See Figure 15
(IS = 3.0 Adc, VGS = 0 Vdc,
dIS/dt = 100 A/
µ
s)
ta
--
32
--
(IS = 3.0 Adc, VGS = 0 Vdc,
dIS/dt = 100 A/
µ
s)
tb
--
44
--
Reverse Recovery Stored Charge
QRR
--
0.133
--
µ
C
(1) Negative sign for PChannel device omitted for clarity.
(2) Pulse Test: Pulse Width
300
µ
s, Duty Cycle
2%.
(3) Switching characteristics are independent of operating junction temperature.
MMSF3P02HD
3
Motorola TMOS Power MOSFET Transistor Device Data
TYPICAL ELECTRICAL CHARACTERISTICS
R
DS(on)
, DRAINT
OSOURCE RESIST
ANCE
(NORMALIZED)
R
DS(on)
, DRAIN-T
O-SOURCE RESIST
ANCE (OHMS)
0
3
4
6
1
5
2
0
0.2
0.4
0.6
0.8
2
0
3
4
6
VDS, DRAINTOSOURCE VOLTAGE (VOLTS)
Figure 1. OnRegion Characteristics
I D
, DRAIN CURRENT
(AMPS)
1.6
1.8
2
2.2
2.4
3.4
I D
, DRAIN CURRENT
(AMPS)
VGS, GATETOSOURCE VOLTAGE (VOLTS)
Figure 2. Transfer Characteristics
0
1
2
3
4
10
0.4
0.6
R
DS(on)
, DRAIN-T
O-SOURCE RESIST
ANCE (OHMS)
0
1
2
3
4
6
0.05
0.07
VGS, GATETOSOURCE VOLTAGE (VOLTS)
Figure 3. OnResistance versus
GateToSource Voltage
ID, DRAIN CURRENT (AMPS)
Figure 4. OnResistance versus Drain Current
and Gate Voltage
0.80
1.20
10
100
1000
TJ, JUNCTION TEMPERATURE (
°
C)
Figure 5. OnResistance Variation with
Temperature
VDS, DRAINTOSOURCE VOLTAGE (VOLTS)
Figure 6. DrainToSource Leakage
Current versus Voltage
I DSS
, LEAKAGE (nA)
TJ = 25
°
C
VDS
10 V
TJ = 100
°
C
25
°
C
55
°
C
VGS = 0 V
ID = 1.5 A
TJ = 25
°
C
VGS = 4.5 V
VGS = 10 V
ID = 3.0 A
1
1.2
3.7 V
3.1 V
2.5 V
2.6
1
1.4
1.6
1.8
2.8
3
3.2
0.2
5
6
7
8
9
10 V
50
0
25
50
75
100
125
150
TJ = 125
°
C
5
0.09
0.06
0.90
2
0
5
1.00
1.10
0
4
8
12
16
20
0.08
2.7 V
2.9 V
VGS = 10 V
3.3 V
3.5 V
3.9 V
4.5 V
TJ = 25
°
C
MMSF3P02HD
4
Motorola TMOS Power MOSFET Transistor Device Data
POWER MOSFET SWITCHING
Switching behavior is most easily modeled and predicted
by recognizing that the power MOSFET is charge controlled.
The lengths of various switching intervals (
t) are deter-
mined by how fast the FET input capacitance can be charged
by current from the generator.
The published capacitance data is difficult to use for calculat-
ing rise and fall because draingate capacitance varies
greatly with applied voltage. Accordingly, gate charge data is
used. In most cases, a satisfactory estimate of average input
current (IG(AV)) can be made from a rudimentary analysis of
the drive circuit so that
t = Q/IG(AV)
During the rise and fall time interval when switching a resis-
tive load, VGS remains virtually constant at a level known as
the plateau voltage, VSGP. Therefore, rise and fall times may
be approximated by the following:
tr = Q2 x RG/(VGG VGSP)
tf = Q2 x RG/VGSP
where
VGG = the gate drive voltage, which varies from zero to VGG
RG = the gate drive resistance
and Q2 and VGSP are read from the gate charge curve.
During the turnon and turnoff delay times, gate current is
not constant. The simplest calculation uses appropriate val-
ues from the capacitance curves in a standard equation for
voltage change in an RC network. The equations are:
td(on) = RG Ciss In [VGG/(VGG VGSP)]
td(off) = RG Ciss In (VGG/VGSP)
The capacitance (Ciss) is read from the capacitance curve at
a voltage corresponding to the offstate condition when cal-
culating td(on) and is read at a voltage corresponding to the
onstate when calculating td(off).
At high switching speeds, parasitic circuit elements com-
plicate the analysis. The inductance of the MOSFET source
lead, inside the package and in the circuit wiring which is
common to both the drain and gate current paths, produces a
voltage at the source which reduces the gate drive current.
The voltage is determined by Ldi/dt, but since di/dt is a func-
tion of drain current, the mathematical solution is complex.
The MOSFET output capacitance also complicates the
mathematics. And finally, MOSFETs have finite internal gate
resistance which effectively adds to the resistance of the
driving source, but the internal resistance is difficult to mea-
sure and, consequently, is not specified.
The resistive switching time variation versus gate resis-
tance (Figure 9) shows how typical switching performance is
affected by the parasitic circuit elements. If the parasitics
were not present, the slope of the curves would maintain a
value of unity regardless of the switching speed. The circuit
used to obtain the data is constructed to minimize common
inductance in the drain and gate circuit loops and is believed
readily achievable with board mounted components. Most
power electronic loads are inductive; the data in the figure is
taken with a resistive load, which approximates an optimally
snubbed inductive load. Power MOSFETs may be safely op-
erated into an inductive load; however, snubbing reduces
switching losses.
GATETOSOURCE OR DRAINTOSOURCE VOLTAGE (Volts)
C, CAP
ACIT
ANCE (pF)
1500
2000
2500
3500
Figure 7. Capacitance Variation
3000
10
0
10
15
20
VGS
VDS
5
5
TJ = 25
°
C
Ciss
Coss
Crss
1000
500
VDS = 0 V
VGS = 0 V
Ciss
Crss
0
MMSF3P02HD
5
Motorola TMOS Power MOSFET Transistor Device Data
Figure 8. GateToSource and DrainToSource
Voltage versus Total Charge
RG, GATE RESISTANCE (OHMS)
1
10
100
1000
100
10
t,
TIME (ns)
VDD = 10 V
ID = 3 A
VGS = 10 V
TJ = 25
°
C
tr
tf
td(off)
td(on)
Figure 9. Resistive Switching Time
Variation versus Gate Resistance
24
V
GS
, GA
TET
OSOURCE VOL
T
AGE (VOL
TS)
20
16
12
8
4
0
0
10
6
2
0
QT, TOTAL CHARGE (nC)
V
DS
, DRAINT
OSOURCE VOL
T
AGE (VOL
TS)
12
8
4
4
8
36
ID = 3 A
TJ = 25
°
C
12
VDS
VGS
QT
Q2
Q3
Q1
16
20
24
28
32
DRAINTOSOURCE DIODE CHARACTERISTICS
The switching characteristics of a MOSFET body diode
are very important in systems using it as a freewheeling or
commutating diode. Of particular interest are the reverse re-
covery characteristics which play a major role in determining
switching losses, radiated noise, EMI and RFI.
System switching losses are largely due to the nature of
the body diode itself. The body diode is a minority carrier de-
vice, therefore it has a finite reverse recovery time, trr, due to
the storage of minority carrier charge, QRR, as shown in the
typical reverse recovery wave form of Figure 15. It is this
stored charge that, when cleared from the diode, passes
through a potential and defines an energy loss. Obviously,
repeatedly forcing the diode through reverse recovery further
increases switching losses. Therefore, one would like a
diode with short trr and low QRR specifications to minimize
these losses.
The abruptness of diode reverse recovery effects the
amount of radiated noise, voltage spikes, and current ring-
ing. The mechanisms at work are finite irremovable circuit
parasitic inductances and capacitances acted upon by high
di/dts. The diode's negative di/dt during ta is directly con-
trolled by the device clearing the stored charge. However,
the positive di/dt during tb is an uncontrollable diode charac-
teristic and is usually the culprit that induces current ringing.
Therefore, when comparing diodes, the ratio of tb/ta serves
as a good indicator of recovery abruptness and thus gives a
comparative estimate of probable noise generated. A ratio of
1 is considered ideal and values less than 0.5 are considered
snappy.
Compared to Motorola standard cell density low voltage
MOSFETs, high cell density MOSFET diodes are faster
(shorter trr), have less stored charge and a softer reverse re-
covery characteristic. The softness advantage of the high
cell density diode means they can be forced through reverse
recovery at a higher di/dt than a standard cell MOSFET
diode without increasing the current ringing or the noise gen-
erated. In addition, power dissipation incurred from switching
the diode will be less due to the shorter recovery time and
lower switching losses.
0.3
0.4
0.5
0.6
0.7
1.4
0
1
2
2.5
3
VSD, SOURCETODRAIN VOLTAGE (VOLTS)
Figure 10. Diode Forward Voltage versus Current
I S
, SOURCE CURRENT
(AMPS)
VGS = 0 V
TJ = 25
°
C
1.5
0.8
0.9
0.5
1
1.1
1.2
1.3