Semiconductor Components Industries, LLC, 2000
November, 2000 – Rev. 1 1Publication Order Number:
MTP7N20E/D
MTP7N20E
Preferred Device
Power MOSFET
7 Amps, 200 Volts
N–Channel TO–220
This Power MOSFET is designed to withstand high energy in the
avalanche and commutation modes. The 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
MAXIMUM RATINGS (TC = 25°C unless otherwise noted)
Rating Symbol Value Unit
Drain–to–Source Voltage VDSS 200 Vdc
Drain–to–Gate Voltage (RGS = 1.0 M) VDGR 200 Vdc
Gate–to–Source Voltage
– Continuous
– Non–Repetitive (tp 10 ms) VGS
VGSM ±20
±40 Vdc
Vpk
Drain Current
– Continuous
– Continuous @ 100°C
– Single Pulse (tp 10 µs)
ID
ID
IDM
7.0
3.8
21
Adc
Apk
Total Power Dissipation @ TC = 25°C
Derate above 25°CPD50
0.4 Watts
W/°C
Operating and Storage Temperature
Range TJ, Tstg –55 to
150 °C
Single Pulse Drain–to–Source Avalanche
Energy – Starting TJ = 25°C
(VDD = 80 Vdc, VGS = 10 Vdc, Peak
IL = 7.0 Adc, L = 10 mH, RG = 25 )
EAS 74 mJ
Thermal Resistance
– Junction to Case°
– Junction to Ambient°RθJC
RθJA 2.5°
62.5°
°C/W
Maximum Lead Temperature for Soldering
Purposes, 1/8 from case for 10
seconds
TL260 °C
7 AMPERES
200 VOLTS
RDS(on) = 700 m
Preferred devices are recommended choices for future use
and best overall value.
Device Package Shipping
ORDERING INFORMATION
MTP7N20E TO–220AB 50 Units/Rail
TO–220AB
CASE 221A
STYLE 5
123
4
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N–Channel
D
S
G
MARKING DIAGRAM
& PIN ASSIGNMENT
MTP7N20E = Device Code
LL = Location Code
Y = Year
WW = Work Week
MTP7N20E
LLYWW
1
Gate 3
Source
4
Drain
2
Drain
MTP7N20E
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2
ELECTRICAL CHARACTERISTICS (TJ = 25°C unless otherwise noted)
Characteristic Symbol Min Typ Max Unit
OFF CHARACTERISTICS
Drain–to–Source Breakdown Voltage
(VGS = 0 Vdc, ID = 0.25 mAdc)
Temperature Coefficient (positive)
V(BR)DSS 200
689
Vdc
mV/°C
Zero Gate Voltage Drain Current
(VDS = 200 Vdc, VGS = 0 Vdc)°
(VDS = 200 Vdc, VGS = 0 Vdc, TJ = 125°C)
IDSS
10
100
µAdc
Gate–Body Leakage Current (VGS = ±20 Vdc, VDS = 0 Vdc) IGSS 100 nAdc
ON CHARACTERISTICS (Note 1.)
Gate Threshold Voltage
(VDS = VGS, ID = 250 µAdc)
Temperature Coefficient (negative)µ
VGS(th) 2.0
3.1
7.1 4.0
Vdc
mV/°C
Static Drain–to–Source On–Resistance (VGS = 10 Vdc, ID = 3.5 Adc) RDS(on) 0.46 0.7 Ohm
Drain–to–Source On–Voltage
(VGS = 10 Vdc, ID = 7.0 Adc)°
(VGS = 10 Vdc, ID = 3.5 Adc, TJ = 125°C)
VDS(on)
3.4
5.9
5.1
Vdc
Forward Transconductance (VDS = 14 Vdc, ID = 3.5 Adc) gFS 1.5 mhos
DYNAMIC CHARACTERISTICS
Input Capacitance
(V 25 Vd V 0 Vd
Ciss 342 480 pF
Output Capacitance (VDS = 25 Vdc, VGS = 0 Vdc,
f=10MHz)
Coss 92 130
Reverse Transfer Capacitance
f
=
1
.
0
MH
z
)
Crss 27 55
SWITCHING CHARACTERISTICS (Note 2.)
Turn–On Delay Time td(on) 8.8 17.6 ns
Rise Time (V
DD
= 100 Vdc, I
D
= 7.0 Adc, tr 29 58
Turn–Of f Delay Time
(VDD
=
100
Vdc
,
ID
=
7
.
0
Adc
,
VGS = 10 Vdc, Rg = 9.1 )td(off) 22 44
Fall Time
GS g )
tf 20 40.8
Gate Charge QT 13.7 21 nC
(See Figure 8)
(
V
DS
= 160 Vdc, I
D
= 7.0 Adc, Q1 3.3
(VDS
=
160
Vdc
,
ID
=
7
.
0
Adc
,
VGS = 10 Vdc) Q2 6.6
GS )
Q3 5.9
SOURCE–DRAIN DIODE CHARACTERISTICS
Forward On–Voltage (Note 1.) (IS = 7.0 Adc, VGS = 0 Vdc)
(IS = 7.0 Adc, VGS = 0 Vdc,
TJ = 125°C)
VSD
1.02
0.9 1.2
Vdc
Reverse Recovery Time trr 138 ns
e e se eco e y e
(See Figure 14)
(I 7 0 Adc V 0 Vdc
ta 93
s
(IS = 7.0 Adc, VGS = 0 Vdc,
dIS/dt
=
100 A/µs)
tb 45
Reverse Recovery Stored
Charge
dI
S
/dt
=
100
A/
µ
s)
QRR 0.74 µC
INTERNAL PACKAGE INDUCTANCE
Internal Drain Inductance
(Measured from contact screw on tab to center of die)
(Measured from the drain lead 0.25 from package to center of die)
Ld
3.5
4.5
nH
Internal Source Inductance
(Measured from the source lead 0.25 from package to source bond pad.) Ls 7.5
1. Pulse Test: Pulse Width 300 µs, Duty Cycle 2.0%.
2. Switching characteristics are independent of operating junction temperature.
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TYPICAL ELECTRICAL CHARACTERISTICS
RDS(on), DRAIN-TO-SOURCE RESISTANCE (OHMS)
Figure 1. On–Region Characteristics Figure 2. Transfer Characteristics
Figure 3. On–Resistance versus Drain Current
and Temperature
ID, DRAIN CURRENT (AMPS)
Figure 4. On–Resistance versus Drain Current
and Gate Voltage
Figure 5. On–Resistance Variation with
Temperature
VDS, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
Figure 6. Drain–To–Source Leakage
Current versus Voltage
IDSS , LEAKAGE (nA)
TJ = 25°C
VGS = 10 V
15 V
0.55
VGS = 0 V
0 100 150
1
100
50 200
TJ = 125°C
0.7
0.65
0.6
10
412826 1410
100°C
D
I , DRAIN CURRENT (AMPS)
8
6
4
2
004 81262
VDS, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
VGS = 10 V
7 V
6 V
8 V
5 V
TJ = 25°C
D
I , DRAIN CURRENT (AMPS)
8
6
4
2
0324 6810
VGS, GATE-TO-SOURCE VOLTAGE (VOLTS)
VDS 10 V -55°C
TJ = 100°C
RDS(on), DRAIN-TO-SOURCE RESISTANCE (OHMS)
1.2
0.8
0.4
002468
ID, DRAIN CURRENT (AMPS)
VGS = 10 V
TJ = 25°C
100°C
-55°C0.5
0.4
0
RDS(on), DRAIN-TO-SOURCE RESISTANCE
(NORMALIZED)
TJ, JUNCTION TEMPERATURE (°C)
VGS = 10 V
ID = 3.5 A
-50 0 50 100 150125-25 25 75
2.5
2
1.5
1
0.5
0
10
10
12
14
9 V
25°C
10
12
14
579
1.0
0.6
0.2
10 12 14
0.45
25°C
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4
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 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
t = Q/IG(AV)
During the rise and fall time interval when switching a
resistive load, VGS remains virtually constant at a level
known a s 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)
The capacitance (Ciss) is read from the capacitance curve a t
a voltage corresponding to the off–state condition when
calculating t d(on) and is read at a voltage corresponding to the
on–state when calculating td(off).
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 a ffected 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.
GATE-TO-SOURCE OR DRAIN-TO-SOURCE VOLTAGE (VOLTS)
Figure 7. Capacitance Variation
C, CAPACITANCE (pF)
10 0 10 15 25
VGS VDS
TJ = 25°C
VDS = 0 V
VGS = 0 V
600
300
020
Ciss
Coss
Crss
55
Ciss
Crss
900
450
150
750
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5
QG, TOTAL GATE CHARGE (nC)
DRAIN–TO–SOURCE DIODE CHARACTERISTICS
VSD, SOURCE-TO-DRAIN VOLTAGE (VOLTS)
Figure 10. Diode Forward Voltage versus Current
IS, SOURCE CURRENT (AMPS)
Figure 9. Resistive Switching Time
Variation versus Gate Resistance
Figure 8. Gate–To–Source and Drain–To–Source
Voltage versus Total Charge
0.5 0.9 1.0
0
7
0.8 1.10.6 0.7
6
3
2
5
4
1
VGS = 0 V
TJ = 25°C
12
10
8
6
4
002 4 6 8 14
180
VDS , DRAIN-TO-SOURCE VOLTAGE (VOLTS
)
VGS , GATE-TO-SOURCE VOLTAGE (VOLTS)
150
90
60
30
0
TJ = 25°C
ID = 7 A
QT
Q2
Q3
VGS
t, TIME (ns)
1000
100
10
11 10 100
RG, GATE RESISTANCE (OHMS)
TJ = 25°C
ID = 7 A
VDS = 100 V
VGS = 10 V
td(off)
td(on)
tf
tr
VDS
10 12
120
2
Q1
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
reliable operation, the stored ener gy 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 (IDM), the energy rating is specified at rated
continuous current (ID), in accordance with industry
custom. The ener gy 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.
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6
SAFE OPERATING AREA
Figure 14. Diode Reverse Recovery Waveform
di/dt
trr
ta
tp
IS
0.25 IS
TIME
IS
tb
Figure 12. Maximum Avalanche Energy versus
Starting Junction Temperature
Figure 11. Maximum Rated Forward Biased
Safe Operating Area
Figure 13. Thermal Response
, SINGLE PULSE DRAIN-TO-SOURCE
AS
E
TJ, STARTING JUNCTION TEMPERATURE (°C)
AVALANCHE ENERGY (mJ)
ID = 7A
80
30
20
10
0
25 50 75 100 125 150
100
10
1
0.1
0.1 1 10 100 1000
100 µs
10 µs
1 ms
10 ms
dc
VDS, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
ID, DRAIN CURRENT (AMPS)
RDS(on) LIMIT
THERMAL LIMIT
PACKAGE LIMIT
VGS = 20 V
SINGLE PULSE
TC = 25°C
1
0.1
0.010.00001 0.0001 0.001 0.01 0.1 1 10
t, TIME (SECONDS)
D = 0.5
0.2
r(t), EFFECTIVE TRANSIENT THERMAL RESISTANCE
(NORMALIZED)
0.1
0.05
0.02
0.01
RθJC(t) = r(t) RθJC
D CURVES APPLY FOR POWER
PULSE TRAIN SHOWN
READ TIME AT t1
TJ(pk) - TC = P(pk) RθJC(t)
P(pk)
t1t2
DUTY CYCLE, D = t1/t2
SINGLE PULSE
40
50
60
70
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7
PACKAGE DIMENSIONS
TO–220 THREE–LEAD
TO–220AB
CASE 221A–09
ISSUE AA
STYLE 5:
PIN 1. GATE
2. DRAIN
3. SOURCE
4. DRAIN
NOTES:
1. DIMENSIONING AND TOLERANCING PER ANSI
Y14.5M, 1982.
2. CONTROLLING DIMENSION: INCH.
3. DIMENSION Z DEFINES A ZONE WHERE ALL
BODY AND LEAD IRREGULARITIES ARE
ALLOWED.
DIM MIN MAX MIN MAX
MILLIMETERSINCHES
A0.570 0.620 14.48 15.75
B0.380 0.405 9.66 10.28
C0.160 0.190 4.07 4.82
D0.025 0.035 0.64 0.88
F0.142 0.147 3.61 3.73
G0.095 0.105 2.42 2.66
H0.110 0.155 2.80 3.93
J0.018 0.025 0.46 0.64
K0.500 0.562 12.70 14.27
L0.045 0.060 1.15 1.52
N0.190 0.210 4.83 5.33
Q0.100 0.120 2.54 3.04
R0.080 0.110 2.04 2.79
S0.045 0.055 1.15 1.39
T0.235 0.255 5.97 6.47
U0.000 0.050 0.00 1.27
V0.045 --- 1.15 ---
Z--- 0.080 --- 2.04
B
Q
H
Z
L
V
G
N
A
K
F
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D
SEATING
PLANE
–T–
C
S
T
U
R
J
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