Motorola MTB75N06HD Datasheet

1
Motorola TMOS Power MOSFET Transistor Device Data
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N–Channel Enhancement–Mode Silicon Gate
The D2PAK package has the capability of housing a larger die than any existing surface mount package which allows it to be used in applications that require the use of surface mount components with higher power and lower R
DS(on)
capabilities. This advanced high–cell density HDTMOS power FET is designed to withstand high energy in the avalanche and commutation modes. This 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 p ower supplies, converters and PWM m otor 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
I
DSS
and V
DS(on)
Specified at Elevated Temperature
Short Heatsink Tab Manufactured — Not Sheared
Specially Designed Leadframe for Maximum Power Dissipation
Available in 24 mm 13–inch/800 Unit Tape & Reel, Add T4 Suffix to Part Number
MAXIMUM RATINGS
(TC = 25°C unless otherwise noted)
Rating Symbol Value Unit
Drain–to–Source Voltage V
DSS
60 Vdc
Drain–to–Gate Voltage (RGS = 1.0 M) V
DGR
60 Vdc
Gate–to–Source Voltage — Continuous
Gate–to–Source Voltage — Non–Repetitive (tp 10 ms)
V
GS
V
GSM
± 20 ± 30
Vdc Vpk
Drain Current — Continuous
Drain Current — Continuous @ 100°C Drain Current — Single Pulse (tp 10 µs)
I
D
I
D
I
DM
75 50
225
Adc
Apk
Total Power Dissipation
Derate above 25°C
Total Power Dissipation @ TC = 25°C (1)
P
D
125
1.0
2.5
Watts
W/°C
Watts Operating and Storage Temperature Range – 55 to 150 °C Single Pulse Drain–to–Source Avalanche Energy — Starting TJ = 25°C
(VDD = 25 Vdc, VGS = 10 Vdc, IL = 75 Apk, L = 0.177 mH, RG = 25 )
E
AS
500 mJ
Thermal Resistance — Junction to Case
Thermal Resistance — Junction to Ambient Thermal Resistance — Junction to Ambient (1)
R
θJC
R
θJA
R
θJA
1.0
62.5 50
°C/W
Maximum Lead Temperature for Soldering Purposes, 1/8″ from case for 10 seconds T
L
260 °C
(1) When surface mounted to an FR4 board using the minimum recommended pad size.
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, Designer’s and HDTMOS are trademarks of Motorola, Inc. TMOS is a registered trademark of Motorola, Inc. Thermal Clad is a trademark of the Bergquist Company.
Preferred devices are Motorola recommended choices for future use and best overall value.
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by MTB75N06HD/D
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SEMICONDUCTOR TECHNICAL DATA
Motorola, Inc. 1995
D
S
G
TMOS POWER FET
75 AMPERES
60 VOLTS
R
DS(on)
= 10 mOHM
Motorola Preferred Device
CASE 418B–02, Style 2
D2PAK
MTB75N06HD
2
Motorola TMOS Power MOSFET Transistor Device Data
ELECTRICAL CHARACTERISTICS
(TJ = 25°C unless otherwise noted)
Characteristic
Symbol Min Typ Max Unit
OFF CHARACTERISTICS
Drain–Source Breakdown Voltage (Cpk 2.0) (3)
(VGS = 0 Vdc, ID = 250 µAdc) Temperature Coefficient (Positive)
V
(BR)DSS
60 —
68
60.4
— —
Vdc
mV/°C
Zero Gate Voltage Drain Current
(VDS = 60 Vdc, VGS = 0 Vdc) (VDS = 60 Vdc, VGS = 0 Vdc, TJ = 125°C)
I
DSS
— —
— —
10
100
µAdc
Gate–Body Leakage Current (VGS = ± 20 Vdc, VDS = 0 V) I
GSS
5.0 100 nAdc
ON CHARACTERISTICS (1)
Gate Threshold Voltage (Cpk 5.0) (3)
(VDS = VGS, ID = 250 µAdc) Temperature Coefficient (Negative)
V
GS(th)
2.0 —
3.0
8.38
4.0 —
Vdc
mV/°C
Static Drain–Source On–Resistance (Cpk 2.0) (3)
(VGS = 10 Vdc, ID = 37.5 Adc)
R
DS(on)
8.3 10
m
Drain–Source On–Voltage (VGS = 10 Vdc)
(ID = 75 Adc) (ID = 37.5 Adc, TJ = 125°C)
V
DS(on)
— —
0.7
0.53
0.9
0.8
Vdc
Forward Transconductance (VDS = 15 Vdc, ID = 37.5 Adc) g
FS
15 32 mhos
DYNAMIC CHARACTERISTICS
Input Capacitance
C
iss
2800 3920 pF
Output Capacitance
(VDS = 25 Vdc, VGS = 0 Vdc,
f = 1.0 MHz)
C
oss
928 1300
Reverse Transfer Capacitance
f = 1.0 MHz)
C
rss
180 252
SWITCHING CHARACTERISTICS (2)
Turn–On Delay Time
t
d(on)
18 26 ns
Rise Time
t
r
218 306
Turn–Off Delay Time
VGS = 10 Vdc,
RG = 9.1 )
t
d(off)
67 94
Fall Time
G
= 9.1 )
t
f
125 175
Q
T
71 100 nC
DS
= 48 Vdc, ID = 75 Adc,
Q
1
16.3
(VDS = 48 Vdc, ID = 75 Adc,
VGS = 10 Vdc)
Q
2
31
Q
3
29.4
SOURCE–DRAIN DIODE CHARACTERISTICS
Forward On–Voltage
(IS = 75 Adc, VGS = 0 Vdc)
(IS = 75 Adc, VGS = 0 Vdc, TJ = 125°C)
V
SD
— —
0.97
0.88
1.1 —
Vdc
t
rr
56
S
= 75 Adc,
t
a
44
(IS = 75 Adc,
dIS/dt = 100 A/µs)
t
b
12
Reverse Recovery Stored Charge Q
RR
0.103 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)
L
D
3.5
nH
Internal Source Inductance
(Measured from the source lead 0.25″ from package to source bond pad)
L
S
7.5 nH
(1) Pulse Test: Pulse Width 300 µs, Duty Cycle 2%. (2) Switching characteristics are independent of operating junction temperature. (3) Reflects typical values.
Cpk =
Max limit – Typ
3 x SIGMA
Gate Charge
Reverse Recovery Time
(VDS = 30 Vdc, ID = 75 Adc,
(V
(I
ns
MTB75N06HD
3
Motorola TMOS Power MOSFET Transistor Device Data
TYPICAL ELECTRICAL CHARACTERISTICS
R
DS(on)
, DRAIN–TO–SOURCE RESISTANCE
(NORMALIZED)
I
DSS
, LEAKAGE (nA)
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS)TJ, JUNCTION TEMPERATURE (°C)
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS) VGS, GATE–TO–SOURCE VOLTAGE (VOLTS)
I
D
, DRAIN CURRENT (AMPS)
I
D
, DRAIN CURRENT (AMPS)
0 0.5 1
Figure 1. On–Region Characteristics Figure 2. Transfer Characteristics
Figure 3. On–Resistance versus Drain Current
and Temperature
Figure 4. On–Resistance versus Drain Current
and Gate Voltage
1
1000
Figure 5. On–Resistance Variation with
Temperature
Figure 6. Drain–To–Source Leakage
Current versus Voltage
VDS ≥ 10 V
TJ = –55°C
25°C
– 50 – 25 0 25 50 75 100 125 150 0 10 20 6040
VGS = 0 V
TJ = 125°C
VGS = 10 V ID = 37.5 A
100
30
9 V
TJ = 25°C
100°C
150
0
21.5
100°C
1.9
1.6
1.3
1
0.7
2 54 73 6 8
125
100
75
50
25
VGS = 10 V
8 V
7 V
6 V
5 V
150
0
125
100
75
50
25
10
50
25°C
R
DS(on)
, DRAIN–TO–SOURCE RESISTANCE (OHMS)
R
DS(on)
, DRAIN–TO–SOURCE RESISTANCE (OHMS)
ID, DRAIN CURRENT (AMPS) ID, DRAIN CURRENT (AMPS)
0 50 150
TJ = 25°C
25 75
15 V
0.016
0.012
0.009
0.007
0.006
0.014
0.012
0.010
0.008
0.006
0.004 100 125
TJ = 25°C VGS = 10 V
TJ = 100°C
25°C
–55°C
VGS = 10 V
0.010
0.008
0 50 15025 75 100 125
0.011
MTB75N06HD
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 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 (I
G(AV)
) can be made from a rudimentary analysis of
the drive circuit so that t = Q/I
G(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, V
SGP
. Therefore, rise and fall times may
be approximated by the following: tr = Q2 x RG/(VGG – V
GSP
)
tf = Q2 x RG/V
GSP
where VGG = the gate drive voltage, which varies from zero to V
GG
RG = the gate drive resistance and Q2 and V
GSP
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:
t
d(on)
= RG C
iss
In [VGG/(VGG – V
GSP
)]
t
d(off)
= RG C
iss
In (VGG/V
GSP
)
The capacitance (C
iss
) is read from the capacitance curve at 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 t
d(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 M OSFET 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.
GATE–TO–SOURCE OR DRAIN–TO–SOURCE VOLTAGE (VOLTS)
C, CAPACITANCE (pF)
Figure 7. Capacitance Variation
10 0 10 15 20 25
V
GS
V
DS
5 5
VDS = 0 V
C
iss
C
rss
VGS = 0 V
TJ = 25°C
C
iss
C
oss
C
rss
7000 6000
5000
4000
3000
2000
1000
0
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