Semiconductor Components Industries, LLC, 2000
November, 2000 – Rev.4 1Publication Order Number:
MTB75N05HD/D
MTB75N05HD
Preferred Device
Power MOSFET
75 Amps, 50 Volts
N–Channel D2PAK
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
Short Heatsink Tab Manufactured – Not Sheared
Specially Designed Leadframe for Maximum Power Dissipation
MAXIMUM RATINGS (TC = 25°C unless otherwise noted)
Rating Symbol Value Unit
Drain–to–Source Voltage VDSS 50 Volts
Drain–to–Gate Voltage (RGS = 1.0 M) VDGR 50
Gate–to–Source Voltage – Continuous VGS ±20
Drain Current – Continuous
Drain Current – Continuous @ 100°C
Drain Current – Single Pulse (tp 10 µs)
ID
ID
IDM
75
65
225
Amps
Total Power Dissipation
Derate above 25°C
Total Power Dissipation @ TA = 25°C
(minimum footprint, FR–4 board)
PD125
1.0
2.5
Watts
W/°C
Watts
Operating and Storage Temperature
Range TJ, Tstg 55 to
150 °C
Single Pulse Drain–to–Source Avalanche
Energy – Starting TJ = 25°C
(VDD = 25 V, VGS = 10 V, Peak
IL = 75 A, L = 0.177 mH, RG = 25 )
EAS 500 mJ
Thermal Resistance
– Junction to Case
– Junction to Ambient
– Junction to Ambient (minimum foot-
print, FR–4 board)
RθJC
RθJA
RθJA
1.0
62.5
50
°C/W
Maximum Temperature for Soldering
Purposes, 1/8 from case for 10
seconds
TL260 °C
MTB75N05HD
YWW
MARKING DIAGRAM
& PIN ASSIGNMENT
MARKING DIAGRAM
& PIN ASSIGNMENT
1
Gate
4
Drain
2
Drain 3
Source
75 AMPERES
50 VOLTS
RDS(on) = 9.5 m
Device Package Shipping
ORDERING INFORMATION
MTB75N05HD D2PAK 50 Units/Rail
D2PAK
CASE 418B
STYLE 2
12
3
4
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N–Channel
D
S
G
MTB75N05HD = Device Code
Y = Year
WW = Work Week
MTB75N05HDT4 D2PAK 800/Tape & Reel
Preferred devices are recommended choices for future use
and best overall value.
MTB75N05HD
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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 (Cpk 2) (Note 2.)
(VGS = 0, ID = 250 µAdc)
Temperature Coefficient (Positive)
V(BR)DSS 50
54.9
Vdc
mV/°C
Zero Gate Voltage Drain Current
(VDS = 50 V, VGS = 0)
(VDS = 50 V, VGS = 0, TJ = 125°C)
IDSS
10
100
µAdc
Gate–Body Leakage Current
(VGS = ±20 Vdc, VDS = 0) IGSS 100 nAdc
ON CHARACTERISTICS (Note 1.)
Gate Threshold Voltage (Cpk 1.5) (Note 2.)
(VDS = VGS, ID = 250 µAdc)
Threshold Temperature Coefficient (Negative)
VGS(th) 2.0
6.3 4.0
Vdc
mV/°C
Static Drain–to–Source On–Resistance (Note 3.) (Cpk 3.0) (Note 2.)
(VGS = 10 Vdc, ID = 20 Adc) RDS(on) 7.0 9.5 m
Drain–to–Source On–Voltage (VGS = 10 Vdc) (Note 3.)
(ID = 75 A)
(ID = 20 Adc, TJ = 125°C)
VDS(on)
0.63
0.34
Vdc
Forward Transconductance (VDS = 10 Vdc, ID = 20 Adc) gFS 15 mhos
DYNAMIC CHARACTERISTICS (Note 2.)
Input Capacitance
(VDS =25VV
GS =0 (C
p
k20)
Ciss 2600 3900 pF
Output Capacitance
(V
DS =
25
V
,
V
GS =
0
,
(C
pk
2
.
0)
f = 1.0 MHz) (Cpk 2.0)
(C )
Coss 1000 1300
Transfer Capacitance
)(
k)
(Cpk 2.0) Crss 230 300
SWITCHING CHARACTERISTICS (Note 4.)
Turn–On Delay Time td(on) 15 30 ns
Rise Time (VDD = 25 V, ID = 75 A,
VGS =10V
tr 170 340
Turn–Of f Delay Time VGS = 10 V,
RG = 9.1 )td(off) 70 140
Fall Time
RG
9.1
)
tf 100 200
Gate Charge QT 71 100 nC
(VDS = 40 V, ID = 75 A, Q1 13
(VDS
40
V
,
ID
75
A
,
VGS = 10 V) Q2 33
Q3 26
SOURCE–DRAIN DIODE CHARACTERISTICS
Forward On–Voltage (Note 2.) (IS = 75 A, VGS = 0) (Cpk 10)
(IS = 20 A, VGS = 0)
(IS = 20 A, VGS = 0, TJ = 125°C)
VSD
0.97
0.80
0.68
1.00
Vdc
Reverse Recovery Time trr 57 ns
(IS = 37.5 A, VGS = 0, ta 40
(IS
37
.
5
A
,
VGS
0
,
dIS/dt = 100 A/µs) tb 17
Reverse Recovery Stored Charge QRR 0.17 µC
INTERNAL PACKAGE INDUCTANCE
Internal Drain Inductance
(Measured from contact screw on tab to center of die)
(Measured from 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%.
2. Reflects Typical Values. Cpk = Absolute Value of (SPEC – AVG) / 3 * SIGMA).
3. For accurate measurements, good Kelvin contact required.
4. Switching characteristics are independent of operating junction temperature.
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TYPICAL ELECTRICAL CHARACTERISTICS (Note 5.)
RDS(on), DRAIN-TO-SOURCE RESISTANCE (OHMS)
RDS(on), DRAIN-TO-SOURCE RESISTANCE
(NORMALIZED) RDS(on), DRAIN-TO-SOURCE RESISTANCE (OHMS)
IDSS, LEAKAGE (nA)
0
160
VDS, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
Figure 1. On–Region Characteristics
ID, DRAIN CURRENT (AMPS)
VGS, GATE-TO-SOURCE VOLTAGE (VOLTS)
Figure 2. Transfer Characteristics
Figure 3. On–Resistance versus Drain Current
and Temperature Figure 4. On–Resistance versus Drain Current
and Gate Voltage
Figure 5. On–Resistance Variation with
Temperature Figure 6. Drain–To–Source Leakage
Current versus Voltage
5 V
TJ = 25°C
100
60
20
012345
160
ID, DRAIN CURRENT (AMPS)
120
80
40
20
00123 5 8
0.014
0.012
0.01
0.006
0.004
0
ID, DRAIN CURRENT (AMPS)
20
TJ = 100°C
25°C
-55°C
VGS = 10 V
0.009
0.008
0.005 0
ID, DRAIN CURRENT (AMPS)
20 40 60 80 100 120
TJ = 25°C
2
1.5
1
0.5
0
-50
TJ, JUNCTION TEMPERATURE (°C)
-25 0 25 50 75 100 125 150
VGS = 10 V
ID = 37.5 A
1000
100
0
VDS, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
015304050
25°C
100°C
VGS = 10 V
TJ = -55°C
25°C
100°C
0.008
0.002
0.007
0.006
140 160
10000
10
40
80
120
140
1.5 2.5 3.5 4.50.5
140
100
60
647
40 60 80 100 120 140
510 2025 35 45
TJ = 125°C
7 V
6 V
5. Pulse Tests: Pulse Width 250 µs, Duty Cycle 2%.
VDS 10 V
15 V
VGS = 10 V
VGS = 0 V
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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 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 a 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)
C, CAPACITANCE (pF)
Figure 7. Capacitance Variation
VGS VDS
8000
10
6000
2000
1000
4000
0
5 0 5 10152025
TJ = 25°C
VDS = 0 VGS = 0
7000
5000
3000
Ciss
Crss
Ciss
Coss
Crss
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Figure 8. Gate–To–Source and Drain–To–Source
Voltage versus Total Charge Figure 9. Resistive Switching Time
Variation versus Gate Resistance
VGS, GATE-TO-SOURCE VOLTAGE (VOLTS)
0
QG, TOTAL GATE CHARGE (nC)
VDS, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
12
t, TIME (ns)
10
8
4
0
25 50
Q1Q2
Q3
1000
100
10
1
RG, GATE RESISTANCE (OHMS)
1 10 100
TJ = 25°C
ID = 75 A
75
TJ = 25°C
ID = 75 A
VDD = 35 V
VGS = 10 V
QT
60
50
40
30
20
10
0
VGS
VDS
2
6
td(off)
td(on)
tr
tf
DRAIN–TO–SOURCE 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
recovery 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
device, 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 12. 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
ringing. 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
controlled by the device clearing the stored charge.
However, the positive di/dt during tb is an uncontrollable
diode characteristic 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 ON Semiconductor standard cell density
low voltage MOSFETs, high cell density MOSFET diodes
are faster (shorter trr), have less stored charge and a softer
reverse recovery 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 generated. In addition, power dissipation incurred
from switching the diode will be less due to the shorter
recovery time and lower switching losses.
0.9
10
20
VSD, SOURCE-TO-DRAIN VOLTAGE (VOLTS)
Figure 10. Diode Forward Voltage versus Current
IS, SOURCE CURRENT (AMPS)
0 0.2 0.4 0.6 0.8 1
80
40
0
TJ = 25°C
VGS = 0 V
0.1 0.3 0.5 0.7
70
60
50
30
IS, SOURCE CURRENT (AMPS)
t, TIME (ns)
Figure 11. Reverse Recovery Time (trr)
40
-120
20
-20
-30
0
-40
-100 -60 -20 20 40 60 80
30
10
-10
-80 -40 0
di/dt = 300 A/µsSTANDARD CELL DENSITY
HIGH CELL DENSITY
tb
trr
ta
trr
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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 that the
transition time (tr, tf) does 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 must be adjusted for operating
conditions d i ffering 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.
0
50
TJ, STARTING JUNCTION TEMPERATURE (°C)
EAS, SINGLE PULSE DRAIN-TO-SOURCE
Figure 12. Maximum Rated Forward Biased
Safe Operating Area
0.1 1 100
VDS, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
Figure 13. Maximum Avalanche Energy versus
Starting Junction Temperature
1
10
100
1000
AVALANCHE ENERGY (mJ)
ID, DRAIN CURRENT (AMPS)
RDS(on) LIMIT
THERMAL LIMIT
PACKAGE LIMIT
0.1 25 50 75 100 12510
VGS = 20 V
SINGLE PULSE
TC = 25°C
500
300
200
100
ID = 75 A
400
100 µs
dc
175150
450
350
250
150
1 ms
10 ms
10 µs
t, TIME (s)
Figure 14. Thermal Response
0.1
1
0.01
1.0E-05 1.0E+01
r(t), EFFECTIVE TRANSIENT THERMAL RESISTANC
E
(NORMALIZED)
RθJC(t) = r(t) RθJC
RθJC = 1.0°C/W MAX
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
0.2
0.05
0.02
0.01
0.1
1.0E-04 1.0E-03 1.0E-02 1.0E-01 1.0E+00
D = 0.5
SINGLE PULSE
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7
0
0.5
1
1.5
2.0
2.5
3
25 50 75 100 125 150
TA, AMBIENT TEMPERATURE (°C)
PD, POWER DISSIPATION (WATTS)
Figure 15. D2PAK Power Derating Curve
RθJA = 50°C/W
Board material = 0.065 mil FR–4
Mounted on the minimum recommended footprint
Collector/Drain Pad Size 450 mils x 350 mils
PACKAGE DIMENSIONS
D2PAK
CASE 418B–03
ISSUE D
STYLE 2:
PIN 1. GATE
2. DRAIN
3. SOURCE
4. DRAIN
NOTES:
1. DIMENSIONING AND TOLERANCING PER ANSI
Y14.5M, 1982.
2. CONTROLLING DIMENSION: INCH.
SEATING
PLANE
S
G
D
–T–
M
0.13 (0.005) T
231
4
3 PL
K
J
H
V
E
C
ADIM MIN MAX MIN MAX
MILLIMETERSINCHES
A0.340 0.380 8.64 9.65
B0.380 0.405 9.65 10.29
C0.160 0.190 4.06 4.83
D0.020 0.035 0.51 0.89
E0.045 0.055 1.14 1.40
G0.100 BSC 2.54 BSC
H0.080 0.110 2.03 2.79
J0.018 0.025 0.46 0.64
K0.090 0.110 2.29 2.79
S0.575 0.625 14.60 15.88
V0.045 0.055 1.14 1.40
–B–
M
B
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MTB75N05HD/D
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