Datasheet MTB2N60E Datasheet (Motorola)

Page 1
1
Motorola TMOS Power MOSFET Transistor Device Data
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N–Channel Enhancement–Mode Silicon Gate
This high voltage MOSFET uses an advanced termination scheme to provide enhanced voltage–blocking capability without degrading performance over time. In addition, 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 high 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.
Robust High Voltage Termination
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
MAXIMUM RATINGS
(TC = 25°C unless otherwise noted)
Rating
Symbol Value Unit
Drain–to–Source Voltage V
DSS
600 Vdc
Drain–to–Gate Voltage (RGS = 1.0 M) V
DGR
600 Vdc
Gate–to–Source Voltage — Continuous
— Non–Repetitive (tp 10 ms)
V
GS
V
GSM
± 20 ± 40
Vdc Vpk
Drain Current — Continuous
— Continuous @ 100°C — Single Pulse (tp 10 µs)
I
D
I
D
I
DM
2.0
1.3
7.0
Adc
Apk
Total Power Dissipation @ 25°C
Derate above 25°C
Total Power Dissipation @ TA = 25°C
(1)
P
D
50
0.4
2.5
Watts
W/°C
Watts
Operating and Storage Temperature Range TJ, T
stg
– 55 to 150 °C
Single Pulse Drain–to–Source Avalanche Energy — Starting TJ = 25°C
(VDD = 50 Vdc, VGS = 10 Vdc, Peak IL = 2.0 Apk, L = 95 mH, RG = 25 )
E
AS
190 mJ
Thermal Resistance — Junction to Case
— Junction to Ambient — Junction to Ambient
(1)
R
θJC
R
θJA
R
θJA
2.5
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 and Designer’s 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.
Order this document
by MTB2N60E/D

SEMICONDUCTOR TECHNICAL DATA
TMOS POWER FET
2.0 AMPERES 600 VOLTS
R
DS(on)
= 3.8 OHM
Motorola Preferred Device
CASE 418B–02, Style 2
D2PAK
D
S
G
Motorola, Inc. 1996
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MTB2N60E
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–to–Source Breakdown Voltage
(VGS = 0 Vdc, ID = 250 µAdc) Temperature Coefficient (Positive)
V
(BR)DSS
600
480
— —
Vdc
mV/°C
Zero Gate Voltage Drain Current
(VDS = 600 Vdc, VGS = 0 Vdc) (VDS = 480 Vdc, VGS = 0 Vdc, TJ = 125°C)
I
DSS
— —
— —
0.25
1.0
µAdc
Gate–Body Leakage Current (VGS = ± 20 Vdc, VDS = 0) I
GSS
100 nAdc
ON CHARACTERISTICS (1)
Gate Threshold Voltage
(VDS = VGS, ID = 250 µAdc) Threshold Temperature Coefficient (Negative)
V
GS(th)
2.0 —
3.1
8.5
4.0 —
Vdc
mV/°C
Static Drain–to–Source On–Resistance (VGS = 10 Vdc, ID = 1.0 Adc) R
DS(on)
3.0 3.8 Ohm
Drain–to–Source On–Voltage
(VGS = 10 Vdc, ID = 2.0 Adc) (VGS = 10 Vdc, ID = 1.0 Adc, TJ = 125°C)
V
DS(on)
— —
— —
8.2
8.4
Vdc
Forward Transconductance (VDS = 50 Vdc, ID = 1.0 Adc) g
FS
1.0 mhos
DYNAMIC CHARACTERISTICS
Input Capacitance
C
iss
435 pF
Output Capacitance
(VDS = 25 Vdc, VGS = 0 Vdc,
f = 1.0 MHz)
C
oss
100
Transfer Capacitance
f = 1.0 MHz)
C
rss
20
SWITCHING CHARACTERISTICS (2)
Turn–On Delay Time
t
d(on)
12 ns
Rise Time
t
r
21
Turn–Off Delay Time
VGS = 10 Vdc,
RG = 18 )
t
d(off)
30
Fall Time
G
= 18 )
t
f
24
Q
T
13 nC
(See Figure 8)
DS
= 400 Vdc, ID = 2.0 Adc,
Q
1
2.0
(VDS = 400 Vdc, ID = 2.0 Adc,
VGS = 10 Vdc)
Q
2
6.0
Q
3
5.0
SOURCE–DRAIN DIODE CHARACTERISTICS
Forward On–Voltage (IS = 2.0 Adc, VGS = 0 Vdc)
(IS = 2.0 Adc, VGS = 0 Vdc, TJ = 125°C)
V
SD
— —
1.0
0.9
1.6 —
Vdc
Reverse Recovery Time (IS = 2.0 Adc, VGS = 0 Vdc,
dIS/dt = 100 A/µs)
t
rr
340
ns
INTERNAL PACKAGE INDUCTANCE
Internal Drain Inductance
(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.
Gate Charge
(VDD = 300 Vdc, ID = 2.0 Adc,
(V
Page 3
MTB2N60E
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Motorola TMOS Power MOSFET Transistor Device Data
TYPICAL ELECTRICAL CHARACTERISTICS
R
DS(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
I
DSS
, LEAKAGE (nA)
TJ = 25°C
VGS = 10 V
15 V
2.9
4.1
3.5
VGS = 0 V
0 200 400
1
100
100 300 600500
TJ = 125°C
1000
3.9
4.3
4.5
3.7
3.3
3.1
10
0.5 1.5 3.52.51 2 43
100°C
D
I , DRAIN CURRENT (AMPS)
4
3
2
1
0
0 4 8 12 16 20
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS)
VGS = 10 V
7 V
6 V
5.5 V
5 V
TJ = 25°C
D
I , DRAIN CURRENT (AMPS)
8
6
4
2
0
0 2 4 6 8 10
VGS, GATE–TO–SOURCE VOLTAGE (VOLTS)
VDS ≥ 10 V
–55°C
TJ = 100°C
25°C
R
DS(on)
, DRAIN–TO–SOURCE RESISTANCE (OHMS)
12
8
4
0
0 1.5 3 4.5 6
ID, DRAIN CURRENT (AMPS)
VGS = 10 V
TJ = 25°C
100°C
–55°C
2.7
2.5 0
R
DS(on)
, DRAIN–TO–SOURCE RESISTANCE
(NORMALIZED)
TJ, JUNCTION TEMPERATURE (°C)
VGS = 10 V ID = 1 A
–50 0 50 100 150125–25 25 75
2.5
2
1.5
1
0.5
0
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MTB2N60E
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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 c omplicates 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)
Figure 7a. Capacitance Variation
Figure 7b. High Voltage Capacitance
Variation
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS)
C, CAPACITANCE (pF)
C
rss
C
iss
C
oss
TJ= 25°C VGS= 0
1000
100
10
1
0.1 10 100 1000
C, CAPACITANCE (pF)
10 0 10 15 25
V
GS
V
DS
TJ = 25
°C
VDS = 0 V VGS = 0 V
600
400
200
0
20
C
iss
C
oss
C
rss
5 5
C
iss
C
rss
800
500
300
100
700
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MTB2N60E
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Motorola TMOS Power MOSFET Transistor Device Data
QG, TOTAL GATE CHARGE (nC)
DRAIN–TO–SOURCE DIODE CHARACTERISTICS
VSD, SOURCE–TO–DRAIN VOLTAGE (VOLTS)
Figure 10. Diode Forward Voltage versus Current
I
S
, 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
0.50 0.70 0.80
0
2.0
0.65 0.75 0.850.55 0.60
1.6
1.2
0.8
0.4
1.8
1.4
1.0
0.6
0.2
VGS = 0 V TJ = 25
°
C
15
12
9
6
3
0
0 4 8 12 16 20
500
V
DS
, DRAIN–TO–SOURCE VOLTAGE (VOLTS)
V
GS
, GATE–TO–SOURCE VOLTAGE (VOLTS)
400
300
200
100
0
V
DS
TJ = 25°C ID = 2 A
Q
T
Q
1
Q
2
Q
3
VDS = 100 V VDS = 250 V VDS = 400 V
V
GS
t, TIME (ns)
1000
100
10
1
1 10 100 1000
RG, GATE RESISTANCE (OHMS)
TJ = 25°C ID = 2 A VDS = 300 V VGS = 10 V
t
d(off)
t
d(on)
t
f t
r
SAFE OPERATING AREA
The Forward Biased Safe Operating Area curves define the maximum simultaneous d rain–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 (V
DSS
) 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 e xceed (T
J(MAX)
– TC)/(R
θJC
).
A Power MOSFET designated E–FET can be safely used
in switching circuits with unclamped inductive loads. For reli-
able 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 p eak current i n avalanche a nd 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 energy rat­ing m ust b e derated for t emperature a s shown i n 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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MTB2N60E
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Motorola TMOS Power MOSFET Transistor Device Data
SAFE OPERATING AREA
Figure 14. Diode Reverse Recovery Waveform
di/dt
t
rr
t
a
t
p
I
S
0.25 I
S
TIME
I
S
t
b
0
0.5
1
1.5
2.0
2.5
3
25 50 75 100 125 150
TA, AMBIENT TEMPERATURE (
°
C)
P
D
, POWER DISSIPATION (WATTS)
Figure 15. D2PAK Power Derating Curve
R
θJA
= 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
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)
Peak IL = 2 A VDD = 50 V
200
150
100
50
0
25 50 75 100 125 150
10
1
0.1
0.01
0.1 1 10 100 1000
100 µs
10 µs
1 ms
10 ms
dc
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS)
I
D
, DRAIN CURRENT (AMPS)
R
DS(on)
LIMIT THERMAL LIMIT PACKAGE LIMIT
VGS = 20 V SINGLE PULSE TC = 25°C
1
0.1
0.01
0.00001 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
R
θ
JC
(t) = r(t) R
θ
JC
D CURVES APPLY FOR POWER PULSE TRAIN SHOWN READ TIME AT t
1
T
J(pk)
– TC = P
(pk)
R
θ
JC
(t)
P
(pk)
t
1
t
2
DUTY CYCLE, D = t1/t
2
SINGLE PULSE
Page 7
MTB2N60E
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Motorola TMOS Power MOSFET Transistor Device Data
INFORMATION FOR USING THE D2PAK SURFACE MOUNT PACKAGE
RECOMMENDED FOOTPRINT FOR SURFACE MOUNTED APPLICATIONS
Surface mount board layout is a critical portion of the total design. The footprint for the semiconductor packages must be the correct size to ensure proper solder connection interface
between the board and the package. With the correct pad geometry, the packages will self align when subjected to a solder reflow process.
mm
inches
0.33
8.38
0.08
2.032
0.04
1.016
0.63
17.02
0.42
10.66
0.12
3.05
0.24
6.096
POWER DISSIPATION FOR A SURFACE MOUNT DEVICE
The power dissipation for a surface mount device is a function of the drain pad size. These can vary from the minimum pad size for soldering to a pad size given for maximum power dissipation. Power dissipation for a surface mount device is determined by T
J(max)
, the maximum rated
junction temperature of the die, R
θJA
, the thermal resistance from the device junction to ambient, and the operating temperature, TA. Using the values provided on the data sheet, PD can be calculated as follows:
PD =
T
J(max)
– T
A
R
θJA
The values for the equation are found in the maximum ratings table on the data sheet. Substituting these values into the equation for an ambient temperature TA of 25°C, one can calculate the power dissipation of the device. For a D2PAK device, PD is calculated as follows.
= 2.5 Watts
The 50°C/W for the D2PAK package assumes the use of the recommended footprint on a glass epoxy printed circuit board to achieve a power dissipation of 2.5 Watts. There are other alternatives to achieving higher power dissipation from the surface mount packages. One is to increase the area of the drain pad. By increasing the area of the drain pad, the power
dissipation can be increased. Although one can almost double the power dissipation with this method, one will be giving up area on the printed circuit board which can defeat the purpose of using surface mount technology. For example, a graph of R
θJA
versus drain pad area is shown in Figure 16.
Thermal Resistance versus Drain Pad
Area for the D2PAK Package (Typical)
2.5 Watts
A, Area (square inches)
Board Material = 0.0625
G–10/FR–4, 2 oz Copper
TA = 25°C
R , Thermal Resistance, Junction
to Ambient ( C/W)
θ
JA
°
60
70
50
40
30
20
1614121086420
3.5 Watts
5 Watts
Another alternative would be to use a ceramic substrate or an aluminum core board such as Thermal Clad. Using a board material such as Thermal Clad, an aluminum core board, the power dissipation can be doubled using the same footprint.
PD =
150°C – 25°C
50°C/W
Figure 16.
Page 8
MTB2N60E
8
Motorola TMOS Power MOSFET Transistor Device Data
SOLDER STENCIL GUIDELINES
Prior to placing surface mount components onto a printed circuit board, solder paste must be applied to the pads. Solder stencils are used to screen the optimum amount. These stencils are typically 0.008 inches thick and may be made of brass or stainless steel. For packages such as the SC–59, SC–70/SOT–323, SOD–123, SOT–23, SOT–143, SOT–223, SO–8, SO–14, SO–16, and SMB/SMC diode packages, the stencil opening should be the same as the pad size or a 1:1 registration. This is not the case with the DPAK and D2PAK packages. If one uses a 1:1 opening to screen solder onto the drain pad, misalignment and/or “tombstoning” may occur due to an excess of solder. For these two packages, the opening in the stencil for the paste should be approximately 50% of the tab area. The opening for the leads is still a 1:1 registration. Figure 17 shows a typical stencil for the DPAK and D2PAK
packages. The pattern of the opening in the stencil for the drain pad is not critical as long as it allows approximately 50% of the pad to be covered with paste.
Figure 17. Typical Stencil for DPAK and
D2PAK Packages
SOLDER PASTE OPENINGS
STENCIL
SOLDERING PRECAUTIONS
The melting temperature of solder is higher than the rated temperature of the device. When the entire device is heated to a high temperature, failure to complete soldering within a short time could result in device failure. Therefore, the following items should always be observed in order to minimize the thermal stress to which the devices are subjected.
Always preheat the device.
The delta temperature between the preheat and soldering
should be 100°C or less.*
When preheating and soldering, the temperature of the
leads and the case must not exceed the maximum temperature ratings as shown on the data sheet. When using infrared heating with the reflow soldering method, the difference shall be a maximum of 10°C.
The soldering temperature and time shall not exceed
260°C for more than 10 seconds.
When shifting from preheating to soldering, the maximum
temperature gradient shall be 5°C or less.
After soldering has been completed, the device should be
allowed to cool naturally for at least three minutes. Gradual cooling should be used as the use of forced cooling will increase the temperature gradient and result in latent failure due to mechanical stress.
Mechanical stress or shock should not be applied during
cooling.
* Soldering a device without preheating can cause excessive thermal shock and stress which can result in damage to the device.
* Due to shadowing and the inability to set the wave height to incorporate other surface mount components, the D2PAK is not recommended for wave soldering.
Page 9
MTB2N60E
9
Motorola TMOS Power MOSFET Transistor Device Data
TYPICAL SOLDER HEATING PROFILE
For any given circuit board, there will be a group of control settings that will give the desired heat pattern. The operator must set temperatures for several heating zones, and a figure for belt speed. T aken together , these control settings make up a heating “profile” for that particular circuit board. On machines controlled by a computer, the computer remembers these profiles from one operating session to the next. Figure 18 shows a typical heating profile for use when soldering a surface mount device to a printed circuit board. This profile will vary among soldering systems but it is a good starting point. Factors that can affect the profile include the type of soldering system in use, density and types of components on the board, type of solder used, and the type of board or substrate material being used. This profile shows temperature versus time. The
line on the graph shows the actual temperature that might be experienced on the surface of a test board at or near a central solder joint. The two profiles are based on a high density and a low density board. The Vitronics SMD310 convection/in­frared reflow soldering system was used to generate this profile. The type of solder used was 62/36/2 Tin Lead Silver with a melting point between 177–189°C. When this type of furnace is used for solder reflow work, the circuit boards and solder joints tend to heat first. The components on the board are then heated by conduction. The circuit board, because it has a large surface area, absorbs the thermal energy more efficiently, then distributes this energy to the components. Because of this effect, the main body of a component may be up to 30 degrees cooler than the adjacent solder joints.
STEP 1
PREHEAT
ZONE 1
“RAMP”
STEP 2
VENT
“SOAK”
STEP 3
HEATING
ZONES 2 & 5
“RAMP”
STEP 4
HEATING
ZONES 3 & 6
“SOAK”
STEP 5
HEATING
ZONES 4 & 7
“SPIKE”
STEP 6
VENT
STEP 7
COOLING
200
°
C
150
°
C
100
°
C
50
°
C
TIME (3 TO 7 MINUTES TOTAL)
T
MAX
SOLDER IS LIQUID FOR
40 TO 80 SECONDS
(DEPENDING ON
MASS OF ASSEMBLY)
205
°
TO 219°C PEAK AT SOLDER JOINT
DESIRED CURVE FOR LOW
MASS ASSEMBLIES
100°C
150°C
160
°
C
170°C
140
°
C
DESIRED CURVE FOR HIGH
MASS ASSEMBLIES
Figure 18. Typical Solder Heating Profile
Page 10
MTB2N60E
10
Motorola TMOS Power MOSFET Transistor Device Data
PACKAGE DIMENSIONS
CASE 418B–02
ISSUE B
NOTES:
1. DIMENSIONING AND TOLERANCING PER ANSI Y14.5M, 1982.
2. CONTROLLING DIMENSION: INCH.
STYLE 2:
PIN 1. GATE
2. DRAIN
3. SOURCE
4. DRAIN
SEATING PLANE
B
S
G
D
–T–
M
0.13 (0.005) T
2 31
4
3 PL
K
J
H
V
E
C
A
DIM MIN MAX MIN MAX
MILLIMETERSINCHES
A 0.340 0.380 8.64 9.65 B 0.380 0.405 9.65 10.29 C 0.160 0.190 4.06 4.83 D 0.020 0.035 0.51 0.89 E 0.045 0.055 1.14 1.40 G 0.100 BSC 2.54 BSC H 0.080 0.110 2.03 2.79 J 0.018 0.025 0.46 0.64 K 0.090 0.110 2.29 2.79 S 0.575 0.625 14.60 15.88 V 0.045 0.055 1.14 1.40
How to reach us: USA /EUROPE: Motorola Literature Distribution; JAPAN: Nippon Motorola Ltd.; Tatsumi–SPD–JLDC, Toshikatsu Otsuki,
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MTB2N60E/D
*MTB2N60E/D
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