MOTOROLA MTW33N10E

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SEMICONDUCTOR TECHNICAL DATA
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Motorola Preferred Device
!
N-Channel Enhancement-Mode Silicon Gate
TMOS POWER FET
33 AMPERES
100 VOLTS
RDS(on) = 0.06 OHM
This advanced TMOS E-FET is designed to withstand high
energy in the avalanche and commutation modes. The new energy
efficient design also offers a drain-to-source diode with a fast
recovery time. Designed for low voltage, high speed switching
applications in power supplies, converters and PWM motor
controls, these devices are particularly well suited for bridge circuits
where diode speed and commutating safe operating areas are
critical and offer additional safety margin against unexpected
voltage transients.
• Avalanche Energy Specified
• Source-to-Drain Diode Recovery Time Comparable to a
Discrete Fast Recovery Diode
• Diode is Characterized for Use in Bridge Circuits
• IDSS and VDS(on) Specified at Elevated Temperature
• Isolated Mounting Hole Reduces Mounting Hardware

D
N-Channel
G
CASE 340F, Style 1
TO-247AE
S
MAXIMUM RATINGS (TJ = 25°C unless otherwise noted)
Rating
Symbol
Value
Unit
Drain-Source Voltage
VDSS
100
Vdc
Drain-Gate Voltage (RGS = 1.0 MΩ)
VDGR
100
Vdc
Gate-Source Voltage — Continuous
Gate-Source Voltage — Non-Repetitive (tp ≤ 10 ms)
VGS
VGSM
± 20
± 40
Vdc
Vpk
Drain Current — Continuous @ 25°C
— Continuous @ 100°C
— Single Pulse (tp ≤ 10 µs)
ID
ID
IDM
33
20
99
Adc
Total Power Dissipation @ TC = 25°C
Derate above 25°C
PD
125
1.0
Watts
W/°C
TJ, Tstg
– 55 to 150
°C
EAS
545
mJ
RθJC
RθJA
1.0
40
°C/W
TL
260
°C
Operating and Storage Temperature Range
Single Pulse Drain-to-Source Avalanche Energy — Starting TJ = 25°C
(VDD = 25 Vdc, VGS = 10 Vdc, IL = 33 Apk, L = 1.000 mH, RG = 25 Ω)
Thermal Resistance — Junction to Case
— Junction to Ambient
Maximum Lead Temperature for Soldering Purposes, 1/8″ from case for 5 seconds
Apk
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.
E-FET and Designer’s are trademarks of Motorola, Inc. TMOS is a registered trademark of Motorola, Inc.
Preferred devices are Motorola recommended choices for future use and best overall value.
3/94
 MTW33N10E
Motorola, Inc. 1994
MTW33N10E
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MOTOROLA
MOTOROLA
1 1
ELECTRICAL CHARACTERISTICS (TC = 25°C unless otherwise noted)
Characteristic
Symbol
Min
Typ
Max
Unit
2.0
—
—
7.0
4.0
—
Vdc
mV/°C
—
0.04
0.06
Ohm
100
—
—
118
—
—
Vdc
mV/°C
—
—
—
—
10
100
—
—
100
—
—
1.6
—
2.4
2.1
gFS
8.0
—
—
mhos
Ciss
—
1830
2500
pF
Coss
—
678
1200
Crss
—
559
1100
td(on)
—
18
40
tr
—
164
330
td(off)
—
48
100
tf
—
83
170
QT
—
52
110
Q1
—
12
—
Q2
—
32
—
Q3
—
24
—
—
—
1.0
0.98
2.0
—
trr
—
144
—
ta
—
108
—
OFF CHARACTERISTICS
Gate Threshold Voltage
(VDS = VGS, ID = 250 µAdc)
Temperature Coefficient (Negative)
VGS(th)
Static Drain-Source On-Resistance (VGS = 10 Vdc, ID = 16.5 Adc)
RDS(on)
Drain-Source Breakdown Voltage
(VGS = 0 Vdc, ID = 250 µAdc)
Temperature Coefficient (Positive)
V(BR)DSS
Zero Gate Voltage Drain Current
(VDS = 100 Vdc, VGS = 0 Vdc)
(VDS = 100 Vdc, VGS = 0 Vdc, TJ = – 25°C)
IDSS
Gate-Body Leakage Current (VGS = ± 20 Vdc, VDS = 0)
IGSS
µAdc
nAdc
ON CHARACTERISTICS (1)
VDS(on)
Drain-Source On-Voltage (VGS = 10 Vdc)
(ID = 33 Adc)
(ID = 16.5 Adc, TJ = – 25°C)
Forward Transconductance (VDS = 8.0 Vdc, ID = 16.5 Adc)
Vdc
DYNAMIC CHARACTERISTICS
Input Capacitance
Output Capacitance
(VDS = 25 Vdc, VGS = 0 Vdc,
f = 1.0 MHz)
Reverse Transfer Capacitance
SWITCHING CHARACTERISTICS (2)
Turn-On Delay Time
Rise Time
Turn-Off Delay Time
(VDD = 50 Vdc, ID = 33 Adc,
VGS = 10 Vdc,
RG = 9.1 Ω)
Fall Time
Gate Charge
(See Figure 8)
(VDS = 80 Vdc, ID = 33 Adc,
VGS = 10 Vdc)
ns
nC
SOURCE-DRAIN DIODE CHARACTERISTICS
Forward On-Voltage (1)
Reverse Recovery Time
(See Figure 14)
(IS = 33 Adc, VGS = 0 Vdc)
(IS = 33 Adc, VGS = 0 Vdc, TJ = 125°C)
(IS = 33 Adc, VGS = 0 Vdc,
dIS/dt = 100 A/µs)
VSD
Vdc
ns
tb
—
36
—
QRR
—
0.93
—
µC
Internal Drain Inductance
(Measured from the drain lead 0.25″ from package to center of die)
LD
—
4.5
—
nH
Internal Source Inductance
(Measured from the source lead 0.25″ from package to source bond pad)
LS
—
13
—
nH
Reverse Recovery Stored Charge
INTERNAL PACKAGE INDUCTANCE
(1) Pulse Test: Pulse Width ≤ 300 µs, Duty Cycle ≤ 2%.
(2) Switching characteristics are independent of operating junction temperature.
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MTW33N10E
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TYPICAL ELECTRICAL CHARACTERISTICS
90
90
TJ = 25°C
VGS = 10 V
9V
70
60
8V
50
40
7V
30
20
6V
10
5V
0
0
1
2
3
5
4
VDS ≥ 10 V
80
I D , DRAIN CURRENT (AMPS)
I D , DRAIN CURRENT (AMPS)
80
6
7
9
8
70
60
25°C
50
100°C
40
30
20
10
0
2.0 2.5 3.0 3.5 4.0 4.5 5.0 5.5 6.0 6.5 7.0 7.5 8.0 8.5 9.0 9.5 10
VGS, GATE-TO-SOURCE VOLTAGE (VOLTS)
10
VDS, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
Figure 2. Transfer Characteristics
R DS(on) , DRAIN-TO-SOURCE RESISTANCE (OHMS)
R DS(on) , DRAIN-TO-SOURCE RESISTANCE (OHMS)
Figure 1. On-Region Characteristics
0.09
VGS = 10 V
0.08
TJ = 100°C
0.07
0.06
0.05
25°C
0.04
– 55°C
0.03
0.02
0
6
12
24
30
36
48
18
42
ID, DRAIN CURRENT (AMPS)
54
60
66
0.053
TJ = 25°C
0.051
0.049
VGS = 10 V
0.047
0.045
0.043
0.041
15 V
0.039
0.037
5
Figure 3. On-Resistance versus Drain Current
and Temperature
17
23
29
35
41
47
ID, DRAIN CURRENT (AMPS)
53
59
65
10000
VGS = 10 V
ID = 16.5 A
VGS = 0 V
1.6
I DSS , LEAKAGE (nA)
RDS(on), DRAIN-TO-SOURCE RESISTANCE
(NORMALIZED)
11
Figure 4. On-Resistance versus Drain Current
and Gate Voltage
2.0
1.8
TJ = – 55°C
1.4
1.2
1.0
TJ = 125°C
1000
100°C
100
25°C
0.8
0.6
–50
–25
0
25
50
75
100
TJ, JUNCTION TEMPERATURE (°C)
125
Figure 5. On-Resistance Variation with
Temperature
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150
10
20
30
40
60
80
50
70
VDS, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
90
Figure 6. Drain-To-Source Leakage
Current versus Voltage
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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 determined by how fast the FET input capacitance can be charged
by current from the generator.
The capacitance (Ciss) is read from the capacitance curve at a
voltage corresponding to the off-state condition when calculating td(on) and is read at a voltage corresponding to the
on-state when calculating td(off).
The published capacitance data is difficult to use for calculating rise and fall because drain-gate 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
At high switching speeds, parasitic circuit elements
complicate 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 function 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 measure and, consequently, is not specified.
The resistive switching time variation versus gate resistance (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
operated into an inductive load; however, snubbing reduces
switching losses.
t = Q/IG(AV)
During the rise and fall time interval when switching a resistive
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 turn-on and turn-off delay times, gate current is not
constant. The simplest calculation uses appropriate values
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)
5000
4000
C, CAPACITANCE (pF)
VDS = 0 V
Ciss
4500
VGS = 0 V
TJ = 25°C
Crss
3500
3000
2500
Ciss
2000
1500
Coss
1000
500
Crss
0
10
5
0
VGS
5
10
15
20
25
VDS
GATE-TO-SOURCE OR DRAIN-TO-SOURCE VOLTAGE (VOLTS)
Figure 7. Capacitance Variation
MOTOROLA
MOTOROLA
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MTW33N10E
MTW33N10E
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VGS
QT
10
100
Q2
8
125
80
Q1
6
60
4
40
Q3
2
0
0
10
VDS
20
30
0
60
50
40
20
1000
VDD = 50 V
ID = 33 A
VGS = 10 V
TJ = 25°C
t, TIME (ns)
ID = 33 A
TJ = 25°C
VDS , DRAIN-TO-SOURCE VOLTAGE (VOLTS)
tr
100
tf
td(off)
10
td(on)
1
10
QG, TOTAL GATE CHARGE (nC)
100
RG, GATE RESISTANCE (OHMS)
Figure 8. Gate-To-Source and Drain-To-Source
Voltage versus Total Charge
Figure 9. Resistive Switching Time
Variation versus Gate Resistance
DRAIN-TO-SOURCE DIODE CHARACTERISTICS
33
30
27
I S , SOURCE CURRENT (AMPS)
VGS, GATE-TO-SOURCE VOLTAGE (VOLTS)
140
14
VGS = 0 V
TJ = 25°C
24
21
18
15
12
9
6
3
0
0.5 0.55
0.6
0.65
0.7
0.75
0.8
0.85
0.9
0.95
1.0
1.05
VSD, SOURCE-TO-DRAIN VOLTAGE (VOLTS)
Figure 10. Diode Forward Voltage versus Current
SAFE OPERATING AREA
The Forward Biased Safe Operating Area curves define
the maximum simultaneous drain-to-source voltage and
drain current that a transistor can handle safely when it is
forward biased. Curves are based upon maximum peak
junction temperature and a case temperature (TC) of 25°C.
Peak repetitive pulsed power limits are determined by using
the thermal response data in conjunction with the procedures
discussed in AN569, “Transient Thermal Resistance-General
Data and Its Use.”
Switching between the off-state and the on-state may
traverse any load line provided neither rated peak current
(IDM) nor rated voltage (VDSS) is exceeded and the transition
time (tr,tf) do not exceed 10 µs. In addition the total power
averaged over a complete switching cycle must not exceed
(TJ(MAX) – TC)/(RθJC).
A Power MOSFET designated E-FET can be safely used
in switching circuits with unclamped inductive loads. For
MTW33N10E
MTW33N10E
5
reliable operation, the stored energy from circuit inductance
dissipated in the transistor while in avalanche must be less
than the rated limit and adjusted for operating conditions
differing from those specified. Although industry practice is to
rate in terms of energy, avalanche energy capability is not a
constant. The energy rating decreases non-linearly with an
increase of peak current in avalanche and peak junction
temperature.
Although many E-FETs can withstand the stress of
drain-to-source avalanche at currents up to rated pulsed
current (I DM ), the energy rating is specified at rated
continuous current (ID), in accordance with industry custom.
The energy rating must be derated for temperature as shown
in the accompanying graph (Figure 12). Maximum energy at
currents below rated continuous ID can safely be assumed to
equal the values indicated.
MOTOROLA
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SAFE OPERATING AREA
550
10 µs
VGS = 20 V
SINGLE PULSE
TC = 25°C
100
10
100 µs
0.0
1 ms
1.0
10 ms
dc
0.1
0.01
RDS(on) LIMIT
THERMAL LIMIT
PACKAGE LIMIT
1.0
0.1
10
500
EAS, SINGLE PULSE DRAIN-TO-SOURCE
AVALANCHE ENERGY (mJ)
I D , DRAIN CURRENT (AMPS)
1000
ID = 33 A
450
400
350
300
250
200
150
100
50
0
25
100
50
75
100
125
150
VDS, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
TJ, STARTING JUNCTION TEMPERATURE (°C)
Figure 11. Maximum Rated Forward Biased
Safe Operating Area
Figure 12. Maximum Avalanche Energy versus
Starting Junction Temperature
r(t), NORMALIZED EFFECTIVE
TRANSIENT THERMAL RESISTANCE
1.0
D = 0.5
0.2
0.1
0.1
P(pk)
0.05
0.02
0.01
t1
t2
DUTY CYCLE, D = t1/t2
SINGLE PULSE
0.01
0.00001
0.0001
0.001
0.01
t,TIME (ms)
0.1
RθJC(t) = r(t) RθJC
D CURVES APPLY FOR POWER
PULSE TRAIN SHOWN
READ TIME AT t1
TJ(pk) – TC = P(pk) RθJC(t)
1.0
10
Figure 13. Thermal Response
di/dt
IS
trr
ta
tb
TIME
0.25 IS
tp
IS
Figure 14. Diode Reverse Recovery Waveform
MOTOROLA
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MTW33N10E
MTW33N10E
PACKAGE DIMENSIONS
φ 0.25 (0.010)
M
T B
M
-T-
-Q-
NOTES:
1. DIMENSIONING AND TOLERANCING PER ANSI
Y14.5M, 1982.
2. CONTROLLING DIMENSION: MILLIMETER.
3. 340F-01 AND -02 OBSOLETE, NEW STANDARD
340F-03.
E
-BC
4
U L
A
STYLE 1:
PIN 1.
2.
3.
4.
R
1
2
3
-Y-
K
P
F
D
0.25 (0.010)
M
Y Q
S
H
V
G
J
GATE
DRAIN
SOURCE
DRAIN
DIM
A
B
C
D
E
F
G
H
J
K
L
P
Q
R
U
V
MILLIMETERS
MIN
MAX
20.40 20.90
15.44 15.95
4.70
5.21
1.09
1.30
1.50
1.63
1.80
2.18
5.45 BSC
2.56
2.87
0.48
0.68
15.57 16.08
7.26
7.50
3.10
3.38
3.50
3.70
3.30
3.80
5.30 BSC
3.05
3.40
INCHES
MIN
MAX
0.803 0.823
0.608 0.628
0.185 0.205
0.043 0.051
0.059 0.064
0.071 0.086
0.215 BSC
0.101 0.113
0.019 0.027
0.613 0.633
0.286 0.295
0.122 0.133
0.138 0.145
0.130 0.150
0.209 BSC
0.120 0.134
CASE 340F-03
MTW33N10E
MTW33N10E
7
MOTOROLA
MOTOROLA
7 7
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