MTD1N80ET4 [MOTOROLA]

1A, 800V, 12ohm, N-CHANNEL, Si, POWER, MOSFET;
MTD1N80ET4
型号: MTD1N80ET4
厂家: MOTOROLA    MOTOROLA
描述:

1A, 800V, 12ohm, N-CHANNEL, Si, POWER, MOSFET

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by MTD1N80E/D  
SEMICONDUCTOR TECHNICAL DATA  
Motorola Preferred Device  
TMOS POWER FET  
1.0 AMPERES  
800 VOLTS  
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.  
R
= 12 OHM  
DS(on)  
D
Robust High Voltage Termination  
Avalanche Energy Specified  
Source–to–Drain Diode Recovery Time Comparable to a Discrete  
Fast Recovery Diode  
G
CASE 369A–13, Style 2  
DPAK  
S
Diode is Characterized for Use in Bridge Circuits  
I
and V Specified at Elevated Temperature  
DSS  
DS(on)  
Surface Mount Package Available in 16 mm, 13–inch/2500  
Unit Tape & Reel, Add T4 Suffix to Part Number  
MAXIMUM RATINGS (T = 25°C unless otherwise noted)  
C
Rating  
Symbol  
Value  
Unit  
Drain–to–Source Voltage  
V
DSS  
800  
Vdc  
Drain–to–Gate Voltage (R  
= 1.0 M)  
V
DGR  
800  
Vdc  
GS  
Gate–to–Source Voltage — Continuous  
Gate–to–Source Voltage — Non–Repetitive (t 10 ms)  
V
± 20  
± 40  
Vdc  
Vpk  
GS  
V
GSM  
p
Drain Current — Continuous  
Drain Current — Continuous @ 100°C  
Drain Current — Single Pulse (t 10 µs)  
I
I
1.0  
0.8  
3.0  
Adc  
Apk  
D
D
I
p
DM  
Total Power Dissipation  
Derate above 25°C  
Total Power Dissipation @ T = 25°C, when mounted to minimum recommended pad size  
P
D
48  
0.38  
1.75  
Watts  
W/°C  
Watts  
A
Operating and Storage Temperature Range  
T , T  
J stg  
55 to 150  
°C  
Single Pulse Drain–to–Source Avalanche Energy — Starting T = 25°C  
E
AS  
mJ  
J
(V  
DD  
= 100 Vdc, V = 10 Vdc, I = 2.0 Apk, L = 10 mH, R = 25 )  
GS L G  
20  
Thermal Resistance — Junction to Case  
Thermal Resistance — Junction to Ambient  
Thermal Resistance — Junction to Ambient, when mounted to minimum recommended pad size  
R
θJC  
R
θJA  
R
θJA  
2.6  
100  
71.4  
°C/W  
Maximum Temperature for Soldering Purposes, 1/8from case for 10 seconds  
T
L
260  
°C  
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.  
REV 1  
Motorola, Inc. 1995  
ELECTRICAL CHARACTERISTICS (T = 25°C unless otherwise noted)  
J
Characteristic  
Symbol  
Min  
Typ  
Max  
Unit  
OFF CHARACTERISTICS  
Drain–to–Source Breakdown Voltage  
V
Vdc  
(BR)DSS  
(V  
= 0 Vdc, I = 0.250 µAdc)  
800  
981  
GS  
D
Temperature Coefficient (Positive)  
mV/°C  
µAdc  
Zero Gate Voltage Drain Current  
I
DSS  
(V  
DS  
(V  
DS  
= 800 Vdc, V  
= 800 Vdc, V  
= 0 Vdc)  
= 0 Vdc, T = 125°C)  
10  
100  
GS  
GS  
J
Gate–Body Leakage Current (V  
= ± 20 Vdc, V  
DS  
= 0 Vdc)  
I
100  
nAdc  
Vdc  
GS  
GSS  
ON CHARACTERISTICS (1)  
Gate Threshold Voltage  
V
GS(th)  
(V  
DS  
= V , I = 250 µAdc)  
2.0  
3.3  
6.3  
4.0  
GS  
D
Temperature Coefficient (Negative)  
Static Drain–to–Source On–Resistance (V  
Drain–to–Source On–Voltage  
mV/°C  
Ohm  
Vdc  
= 10 Vdc, I = 0.5 Adc)  
R
V
10.3  
12  
GS  
D
DS(on)  
DS(on)  
(V  
GS  
(V  
GS  
= 10 Vdc, I = 1.0 Adc)  
11  
14.4  
12.6  
D
= 10 Vdc, I = 0.5 Adc, T = 125°C)  
D
J
Forward Transconductance (V  
DS  
= 15 Vdc, I = 0.5 Adc)  
g
0.4  
0.985  
mhos  
pF  
D
FS  
DYNAMIC CHARACTERISTICS  
Input Capacitance  
C
297  
29  
420  
40  
iss  
(V  
DS  
= 25 Vdc, V = 0 Vdc,  
GS  
Output Capacitance  
C
oss  
f = 1.0 MHz)  
Reverse Transfer Capacitance  
C
6.0  
10  
rss  
SWITCHING CHARACTERISTICS (2)  
Turn–On Delay Time  
t
9.0  
10  
20  
20  
40  
55  
20  
ns  
d(on)  
(V  
= 400 Vdc, I = 1.0 Adc,  
D
Rise Time  
DD  
DS  
t
r
V
= 10 Vdc,  
GS  
G
Turn–Off Delay Time  
Fall Time  
t
20  
d(off)  
R
= 9.1 )  
t
f
27  
Gate Charge  
Q
T
Q
1
Q
2
Q
3
9.6  
2.1  
4.2  
4.7  
nC  
(V  
= 400 Vdc, I = 1.0 Adc,  
D
V
GS  
= 10 Vdc)  
SOURCE–DRAIN DIODE CHARACTERISTICS  
Forward On–Voltage (1)  
V
Vdc  
ns  
SD  
(I = 1.0 Adc, V  
(I = 1.0 Adc, V  
GS  
= 0 Vdc)  
= 0 Vdc, T = 125°C)  
S
GS  
0.82  
0.7  
1.2  
S
J
Reverse Recovery Time  
t
317  
56  
rr  
t
a
(I = 1.0 Adc, V  
= 0 Vdc,  
dI /dt = 100 A/µs)  
S
GS  
S
t
261  
0.93  
b
Reverse Recovery Stored Charge  
Q
µC  
RR  
INTERNAL PACKAGE INDUCTANCE  
Internal Drain Inductance  
(Measured from the drain lead 0.25from package to center of die)  
L
nH  
nH  
D
4.5  
7.5  
Internal Source Inductance  
(Measured from the source lead 0.25from package to source bond pad)  
L
S
(1) Pulse Test: Pulse Width 300 µs, Duty Cycle 2%.  
(2) Switching characteristics are independent of operating junction temperature.  
2
Motorola TMOS Power MOSFET Transistor Device Data  
TYPICAL ELECTRICAL CHARACTERISTICS  
2.0  
1.6  
2.0  
T
= 25°C  
J
V
DS  
10 V  
1.6  
1.2  
0.8  
V
= 10 V  
GS  
6 V  
8 V  
1.2  
0.8  
5 V  
T
= 100°C  
J
0.4  
0
0.4  
0
25°C  
4 V  
–55  
5.0  
, GATE–TO–SOURCE VOLTAGE (VOLTS)  
°C  
0
5
10  
15  
20  
2.0  
2.5  
3.0  
GS  
3.5  
4.0  
4.5  
5.5  
6.0  
V
, DRAIN–TO–SOURCE VOLTAGE (VOLTS)  
V
DS  
Figure 1. On–Region Characteristics  
Figure 2. Transfer Characteristics  
16  
18  
15  
12  
9
V
= 10 V  
GS  
T
= 25°C  
J
15  
14  
13  
12  
11  
10  
9
100°C  
T
= 25°C  
J
V
= 10 V  
GS  
6
–55°C  
15 V  
3
0
0
0.25  
0.50  
0.75  
1.0  
1.25  
1.50  
1.75  
2.0  
0
0.4  
0.8  
1.2  
1.6  
2.0  
I
, DRAIN CURRENT (AMPS)  
I
, DRAIN CURRENT (AMPS)  
D
D
Figure 3. On–Resistance versus Drain Current  
and Temperature  
Figure 4. On–Resistance versus Drain Current  
and Gate Voltage  
2.5  
1000  
V
= 10 V  
V
= 0 V  
GS  
= 0.5 A  
GS  
I
D
T
= 125°C  
J
2
100  
100°C  
1.5  
10  
1
1
0.5  
0
25°C  
0.1  
50  
25  
0
25  
50  
75  
100  
C)  
125  
150  
0
100  
200  
300  
400  
500  
600  
700  
800  
T , JUNCTION TEMPERATURE (  
°
J
V
, DRAIN–TO–SOURCE VOLTAGE (VOLTS)  
DS  
Figure 5. On–Resistance Variation with  
Temperature  
Figure 6. Drain–To–Source Leakage  
Current versus Voltage  
Motorola TMOS Power MOSFET Transistor Device Data  
3
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 deter-  
mined by how fast the FET input capacitance can be charged  
by current from the generator.  
The capacitance (C ) is read from the capacitance curve at  
a voltage corresponding to the off–state condition when cal-  
iss  
culating t  
and is read at a voltage corresponding to the  
d(on)  
on–state when calculating t  
.
d(off)  
At high switching speeds, parasitic circuit elements com-  
plicate 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 func-  
tion 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 mea-  
sure and, consequently, is not specified.  
The resistive switching time variation versus gate resis-  
tance (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 op-  
erated into an inductive load; however, snubbing reduces  
switching losses.  
The published capacitance data is difficult to use for calculat-  
ing 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  
the drive circuit so that  
) can be made from a rudimentary analysis of  
G(AV)  
t = Q/I  
G(AV)  
During the rise and fall time interval when switching a resis-  
tive load, V remains virtually constant at a level known as  
GS  
the plateau voltage, V  
. Therefore, rise and fall times may  
SGP  
be approximated by the following:  
t = Q x R /(V  
– V )  
GSP  
r
2
G
GG  
t = Q x R /V  
f
2
G
GSP  
where  
V
= the gate drive voltage, which varies from zero to V  
= the gate drive resistance  
GG  
GG  
R
G
and Q and V  
GSP  
are read from the gate charge curve.  
2
During the turn–on and turn–off delay times, gate current is  
not constant. The simplest calculation uses appropriate val-  
ues from the capacitance curves in a standard equation for  
voltage change in an RC network. The equations are:  
t
t
= R  
= R  
C
C
In [V  
/(V  
GG GG  
– V  
)]  
GSP  
d(on)  
G
iss  
In (V  
/V  
)
d(off)  
G
iss  
GG GSP  
1000  
700  
600  
T
J
GS  
= 25°C  
= 0  
T
= 25°C  
J
V
C
V
= 0 V  
iss  
GS  
500  
400  
300  
200  
100  
0
100  
10  
1
C
iss  
C
oss  
C
rss  
C
oss  
C
rss  
0
5
10  
15  
20  
25  
10  
100  
1000  
GATE–TO–SOURCE OR DRAIN–TO–SOURCE VOLTAGE (VOLTS)  
V
, DRAIN–TO–SOURCE VOLTAGE (VOLTS)  
DS  
Figure 7a. Capacitance Variation  
Figure 7b. High Voltage Capacitance Variation  
4
Motorola TMOS Power MOSFET Transistor Device Data  
100  
12  
10  
400  
300  
V
= 400 V  
= 1 A  
= 10 V  
= 25°C  
DD  
QT  
I
V
T
D
GS  
V
J
GS  
t
f
8
6
4
2
0
t
d(off)  
10  
200  
100  
0
t
d(on)  
t
r
Q1  
Q2  
I
T
= 1 A  
= 25°C  
D
J
V
DS  
Q3  
1
0
2
4
6
8
10  
1
10  
R , GATE RESISTANCE (OHMS)  
G
100  
Q , TOTAL CHARGE (nC)  
T
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  
1.0  
V
= 0 V  
GS  
= 25°C  
T
J
0.8  
0.6  
0.4  
0.2  
0
0.40 0.45  
0.50  
0.55 0.60 0.65  
0.70 0.75  
0.80 0.85  
V
, SOURCE–TO–DRAIN VOLTAGE (VOLTS)  
SD  
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 for-  
ward biased. Curves are based upon maximum peak junc-  
able operation, the stored energy from circuit inductance dis-  
sipated 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 con-  
stant. The energy rating decreases non–linearly with an in-  
crease of peak current in avalanche and peak junction  
temperature.  
tion temperature and a case temperature (T ) of 25°C. Peak  
C
repetitive pulsed power limits are determined by using the  
thermal response data in conjunction with the procedures  
discussed in AN569, “Transient Thermal Resistance–Gener-  
al Data and Its Use.”  
Although many E–FETs can withstand the stress of drain–  
to–source avalanche at currents up to rated pulsed current  
Switching between the off–state and the on–state may tra-  
verse any load line provided neither rated peak current (I  
)
DM  
) is exceeded and the transition time  
(I  
), the energy rating is specified at rated continuous cur-  
DM  
nor rated voltage (V  
DSS  
rent (I ), in accordance with industry custom. The energy rat-  
D
(t ,t ) do not exceed 10 µs. In addition the total power aver-  
r f  
ing must be derated for temperature as shown in the  
accompanying graph (Figure 12). Maximum energy at cur-  
aged over a complete switching cycle must not exceed  
(T  
– T )/(R ).  
J(MAX)  
C
θJC  
rents below rated continuous I can safely be assumed to  
A Power MOSFET designated E–FET can be safely used  
D
in switching circuits with unclamped inductive loads. For reli-  
Motorola TMOS Power MOSFET Transistor Device Data  
equal the values indicated.  
5
SAFE OPERATING AREA  
20  
10  
1
V
= 20 V  
GS  
SINGLE PULSE  
= 25  
I
= 1 A  
D
10 µs  
T
°C  
C
15  
10  
5
100 µs  
1 ms  
10 ms  
dc  
0.1  
R
LIMIT  
DS(on)  
THERMAL LIMIT  
PACKAGE LIMIT  
0.01  
0
0.1  
1
10  
100  
1000  
25  
50  
75  
100  
125  
C)  
150  
T , STARTING JUNCTION TEMPERATURE (  
°
J
V
, DRAIN–TO–SOURCE VOLTAGE (VOLTS)  
DS  
Figure 11. Maximum Rated Forward Biased  
Safe Operating Area  
Figure 12. Maximum Avalanche Energy versus  
Starting Junction Temperature  
1
D = 0.5  
0.2  
0.1  
0.1  
0.05  
P
(pk)  
R
(t) = r(t) R  
JC θJC  
θ
0.02  
0.01  
SINGLE PULSE  
D CURVES APPLY FOR POWER  
PULSE TRAIN SHOWN  
READ TIME AT t  
t
1
1
t
T
– T = P  
R (t)  
(pk) θJC  
2
J(pk)  
C
DUTY CYCLE, D = t /t  
1 2  
0.01  
0.00001  
0.0001  
0.001  
0.01  
t, TIME (SECONDS)  
0.1  
1
10  
Figure 13. Thermal Response  
di/dt  
I
S
t
rr  
t
t
a
b
TIME  
0.25 I  
t
S
p
I
S
Figure 14. Diode Reverse Recovery Waveform  
6
Motorola TMOS Power MOSFET Transistor Device Data  
INFORMATION FOR USING THE DPAK SURFACE MOUNT PACKAGE  
RECOMMENDED FOOTPRINTS 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.  
0.165  
4.191  
0.118  
3.0  
0.100  
2.54  
0.063  
1.6  
0.190  
4.826  
0.243  
6.172  
inches  
mm  
POWER DISSIPATION FOR A SURFACE MOUNT DEVICE  
The power dissipation for a surface mount device is a  
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  
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  
junction temperature of the die, R  
θJA  
, the maximum rated  
, the thermal resistance  
R
versus drain pad area is shown in Figure 15.  
J(max)  
θJA  
from the device junction to ambient, and the operating  
temperature, T . Using the values provided on the data sheet,  
100  
Board Material = 0.0625  
A
G–10/FR–4, 2 oz Copper  
P
can be calculated as follows:  
D
1.75 Watts  
80  
60  
40  
20  
T
= 25°C  
T
– T  
A
A
J(max)  
P
=
D
R
θJA  
3.0 Watts  
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 T of 25°C, one can  
calculate the power dissipation of the device. For a DPAK  
A
5.0 Watts  
device, P is calculated as follows.  
D
0
2
4
6
8
10  
150°C – 25°C  
= 1.75 Watts  
P
=
D
A, AREA (SQUARE INCHES)  
71.4°C/W  
Figure 15. Thermal Resistance versus Drain Pad  
Area for the DPAK Package (Typical)  
The 71.4°C/W for the DPAK package assumes the use of  
the recommended footprint on a glass epoxy printed circuit  
board to achieve a power dissipation of 1.75 Watts. There are  
other alternatives to achieving higher power dissipation from  
thesurfacemountpackages. Oneistoincreasetheareaofthe  
drain pad. By increasing the area of the drain pad, the power  
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.  
Motorola TMOS Power MOSFET Transistor Device Data  
7
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  
SOLDER PASTE  
OPENINGS  
2
STENCIL  
registration. This is not the case with the DPAK and D PAK  
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 16. Typical Stencil for DPAK and  
2
D PAK Packages  
2
Figure 16 shows a typical stencil for the DPAK and D PAK  
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.  
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.  
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.  
Always preheat the device.  
The delta temperature between the preheat and soldering  
should be 100°C or less.*  
Mechanical stress or shock should not be applied during  
cooling.  
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.  
* 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  
2
The soldering temperature and time shall not exceed  
260°C for more than 10 seconds.  
incorporate other surface mount components, the D PAK is  
not recommended for wave soldering.  
8
Motorola TMOS Power MOSFET Transistor Device Data  
TYPICAL SOLDER HEATING PROFILE  
For any given circuit board, there will be a group of control  
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/in-  
frared 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 177189°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.  
settings that will give the desired heat pattern. The operator  
must set temperatures for several heating zones, and a figure  
for belt speed. Taken 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  
17 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,  
typeofsolderused, andthetypeofboardorsubstratematerial  
being used. This profile shows temperature versus time. The  
STEP 5  
HEATING  
ZONES 4 & 7  
“SPIKE”  
STEP 6  
VENT  
STEP 7  
COOLING  
STEP 1  
PREHEAT  
ZONE 1  
“RAMP”  
STEP 4  
HEATING  
ZONES 3 & 6  
“SOAK”  
STEP 2  
VENT  
“SOAK” ZONES 2 & 5  
“RAMP”  
STEP 3  
HEATING  
205  
PEAK AT  
SOLDER JOINT  
° TO 219°C  
200  
°
C
C
170°C  
DESIRED CURVE FOR HIGH  
MASS ASSEMBLIES  
160°C  
150°C  
150°  
SOLDER IS LIQUID FOR  
40 TO 80 SECONDS  
(DEPENDING ON  
100°C  
140°C  
MASS OF ASSEMBLY)  
100  
°
C
C
DESIRED CURVE FOR LOW  
MASS ASSEMBLIES  
50°  
TIME (3 TO 7 MINUTES TOTAL)  
T
MAX  
Figure 17. Typical Solder Heating Profile  
Motorola TMOS Power MOSFET Transistor Device Data  
9
PACKAGE DIMENSIONS  
NOTES:  
1. DIMENSIONING AND TOLERANCING PER ANSI  
Y14.5M, 1982.  
SEATING  
PLANE  
–T–  
2. CONTROLLING DIMENSION: INCH.  
C
B
R
INCHES  
MILLIMETERS  
E
V
DIM  
A
B
C
D
E
MIN  
MAX  
0.250  
0.265  
0.094  
0.035  
0.040  
0.047  
MIN  
5.97  
6.35  
2.19  
0.69  
0.84  
0.94  
MAX  
6.35  
6.73  
2.38  
0.88  
1.01  
1.19  
0.235  
0.250  
0.086  
0.027  
0.033  
0.037  
Z
A
K
S
F
G
H
J
K
L
0.180 BSC  
4.58 BSC  
U
0.034  
0.018  
0.102  
0.040  
0.023  
0.114  
0.87  
0.46  
2.60  
1.01  
0.58  
2.89  
0.090 BSC  
2.29 BSC  
F
J
R
S
U
V
0.175  
0.020  
0.020  
0.030  
0.138  
0.215  
0.050  
–––  
0.050  
–––  
4.45  
0.51  
0.51  
0.77  
3.51  
5.46  
1.27  
–––  
1.27  
–––  
STYLE 2:  
PIN 1. GATE  
2. DRAIN  
L
H
D 2 PL  
0.13 (0.005)  
Z
3. SOURCE  
4. DRAIN  
M
G
T
CASE 369A–13  
ISSUE W  
Motorolareserves the right to make changes without further notice to any products herein. Motorola makes no warranty, representationorguaranteeregarding  
the suitability of its products for any particular purpose, nor does Motorola assume any liability arising out of the application or use of any product or circuit,  
andspecifically disclaims any and all liability, includingwithoutlimitationconsequentialorincidentaldamages. “Typical” parameters can and do vary in different  
applications. All operating parameters, including “Typicals” must be validated for each customer application by customer’s technical experts. Motorola does  
not convey any license under its patent rights nor the rights of others. Motorola products are not designed, intended, or authorized for use as components in  
systems intended for surgical implant into the body, or other applications intended to support or sustain life, or for any other application in which the failure of  
the Motorola product could create a situation where personal injury or death may occur. Should Buyer purchase or use Motorola products for any such  
unintendedor unauthorized application, Buyer shall indemnify and hold Motorola and its officers, employees, subsidiaries, affiliates, and distributors harmless  
against all claims, costs, damages, and expenses, and reasonable attorney fees arising out of, directly or indirectly, any claim of personal injury or death  
associated with such unintended or unauthorized use, even if such claim alleges that Motorola was negligent regarding the design or manufacture of the part.  
Motorola and  
are registered trademarks of Motorola, Inc. Motorola, Inc. is an Equal Opportunity/Affirmative Action Employer.  
How to reach us:  
USA / EUROPE: Motorola Literature Distribution;  
JAPAN: Nippon Motorola Ltd.; Tatsumi–SPD–JLDC, Toshikatsu Otsuki,  
P.O. Box 20912; Phoenix, Arizona 85036. 1–800–441–2447  
6F Seibu–Butsuryu–Center, 3–14–2 Tatsumi Koto–Ku, Tokyo 135, Japan. 03–3521–8315  
MFAX: RMFAX0@email.sps.mot.com – TOUCHTONE (602) 244–6609  
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MTD1N80E/D  

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