MTB16N25E [ROCHESTER]

16A, 250V, 0.25ohm, N-CHANNEL, Si, POWER, MOSFET, CASE 418B-02, D2PAK-3;
MTB16N25E
型号: MTB16N25E
厂家: Rochester Electronics    Rochester Electronics
描述:

16A, 250V, 0.25ohm, N-CHANNEL, Si, POWER, MOSFET, CASE 418B-02, D2PAK-3

文件: 总12页 (文件大小:958K)
中文:  中文翻译
下载:  下载PDF数据表文档文件
MTB16N25E  
Designer’sData Sheet  
TMOS E−FET.™  
High Energy Power FET  
D2PAK for Surface Mount  
NChannel EnhancementMode Silicon  
Gate  
http://onsemi.com  
TMOS POWER FET  
16 AMPERES, 250 VOLTS  
2
The D PAK 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  
R
DS(on) = 0.25 OHM  
higher power and lower R  
capabilities. This advanced TMOS  
DS(on)  
EFET is designed to withstand high energy in the avalanche and  
commutation modes. The new energy efficient design also offers a  
draintosource 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.  
CASE 418B02, Style 2  
2
D PAK  
Avalanche Energy Specified  
SourcetoDrain Diode Recovery Time Comparable to a  
Discrete Fast Recovery Diode  
D
Diode is Characterized for Use in Bridge Circuits  
I  
and V  
Specified at Elevated Temperature  
DSS  
DS(on)  
G
Short Heatsink Tab Manufactured — Not Sheared  
Specially Designed Leadframe for Maximum Power Dissipation  
Available in 24 mm 13inch/800 Unit Tape & Reel, Add T4  
Suffix to Part Number  
®
S
© Semiconductor Components Industries, LLC, 2006  
1
Publication Order Number:  
August, 2006 Rev. 1  
MTB16N25E/D  
MTB16N25E  
MAXIMUM RATINGS (T = 25°C unless otherwise noted)  
C
Rating  
Symbol  
Value  
250  
Unit  
Vdc  
Vdc  
DrainSource Voltage  
V
DSS  
DGR  
DrainGate Voltage (R = 1.0 MΩ)  
V
V
250  
GS  
GateSource Voltage — Continuous  
V
GS  
± 20  
± 40  
Vdc  
Vpk  
GateSource Voltage — NonRepetitive (t 10 ms)  
p
GSM  
Drain Current — Continuous  
Drain Current — Continuous @ T = 100°C  
Drain Current — Single Pulse (t 10 μs)  
I
I
16  
10  
56  
Adc  
D
C
D
I
Apk  
p
DM  
Total Power Dissipation @ T = 25°C  
Derate above 25°C  
P
D
125  
1.0  
2.5  
Watts  
W/°C  
Watts  
C
Total Power Dissipation @ T = 25°C, when mounted with the minimum recommended pad size  
A
Operating and Storage Temperature Range  
T , T  
55 to 150  
°C  
J
stg  
Single Pulse DraintoSource Avalanche Energy — Starting T = 25°C  
E
AS  
384  
mJ  
J
(V = 80 Vdc, V = 10 Vdc, I = 16 Apk, L = 3.0 mH, R = 25 Ω )  
DD  
GS  
L
G
Thermal Resistance — Junction to Case  
Thermal Resistance — Junction to Ambient  
Thermal Resistance — Junction to Ambient, when mounted with the minimum recommended pad size  
R
R
R
1.0  
62.5  
50  
°C/W  
θ
JC  
JA  
JA  
θ
θ
Maximum Lead 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.  
EFET 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.  
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MTB16N25E  
ELECTRICAL CHARACTERISTICS (T = 25°C unless otherwise noted)  
J
Characteristic  
Symbol  
Min  
Typ  
Max  
Unit  
OFF CHARACTERISTICS  
DrainSource Breakdown Voltage  
V
(BR)DSS  
(V = 0 Vdc, I = 250 μAdc)  
Temperature Coefficient (Positive)  
250  
333  
Vdc  
mV/°C  
GS  
D
Zero Gate Voltage Drain Current  
I
μAdc  
DSS  
(V = 250 Vdc, V = 0 Vdc)  
10  
100  
DS  
GS  
(V = 250 Vdc, V = 0 Vdc, T = 125°C)  
DS  
GS  
J
GateBody Leakage Current (V = ± 20 Vdc, V = 0)  
I
100  
nAdc  
GS  
DS  
GSS  
ON CHARACTERISTICS (1)  
Gate Threshold Voltage  
V
GS(th)  
(V = V , I = 250 μAdc)  
Temperature Coefficient (Negative)  
2.0  
3.0  
7.0  
4.0  
Vdc  
mV/°C  
DS  
GS  
D
Static DrainSource OnResistance (V = 10 Vdc, I = 8.0 Adc)  
R
V
0.17  
0.25  
Ohm  
Vdc  
GS  
D
DS(on)  
DrainSource OnVoltage (V = 10 Vdc)  
GS  
DS(on)  
(I = 16 Adc)  
(I = 8.0 Adc, T = 125°C)  
D
3.6  
4.8  
4.2  
D
J
Forward Transconductance (V = 15 Vdc, I = 8.0 Adc)  
g
FS  
3.0  
7.0  
mhos  
pF  
DS  
D
DYNAMIC CHARACTERISTICS  
Input Capacitance  
C
1558  
281  
2180  
390  
iss  
(V = 25 Vdc, V = 0 Vdc,  
DS  
GS  
Output Capacitance  
C
oss  
f = 1.0 MHz)  
Reverse Transfer Capacitance  
C
130  
260  
rss  
SWITCHING CHARACTERISTICS (2)  
TurnOn Delay Time  
t
15  
64  
30  
130  
110  
90  
ns  
d(on)  
(V = 125 Vdc, I = 16 Adc,  
DD  
D
Rise Time  
t
r
V
GS  
= 10 Vdc,  
TurnOff Delay Time  
Fall Time  
t
56  
d(off)  
R
= 9.1 Ω)  
G
t
f
44  
Gate Charge  
(See Figure 8)  
Q
T
Q
1
Q
2
Q
3
53.4  
9.3  
27.5  
17.1  
70  
nC  
(V = 200 Vdc, I = 16 Adc,  
DS  
D
V
GS  
= 10 Vdc)  
SOURCEDRAIN DIODE CHARACTERISTICS  
Forward OnVoltage (1)  
V
Vdc  
ns  
SD  
(I = 16 Adc, V = 0 Vdc)  
S
GS  
0.915  
1.39  
1.5  
(I = 16 Adc, V = 0 Vdc, T = 125°C)  
S
GS  
J
Reverse Recovery Time  
(See Figure 14)  
t
234  
170  
rr  
t
a
(I = 16 Adc, V = 0 Vdc,  
S
GS  
dI /dt = 100 A/μs)  
S
t
64  
b
Reverse Recovery Stored Charge  
Q
2.165  
μC  
RR  
INTERNAL PACKAGE INDUCTANCE  
Internal Drain Inductance  
(Measured from the drain lead 0.25from package to center of die)  
L
4.5  
7.5  
nH  
nH  
D
Internal Source Inductance  
L
S
(Measured from the source lead 0.25from package to source bond pad)  
(1) Pulse Test: Pulse Width 300 μs, Duty Cycle 2%.  
(2) Switching characteristics are independent of operating junction temperature.  
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3
MTB16N25E  
TYPICAL ELECTRICAL CHARACTERISTICS  
32  
24  
16  
32  
V
GS  
= 10 V  
T = 25°C  
J
V
DS  
10 V  
8 V  
7 V  
24  
16  
25°C  
6 V  
100°C  
8
0
8
0
5 V  
T = −55°C  
J
0
1
2
3
4
5
6
7
8
2
3
4
5
6
7
V
DS  
, DRAIN−TO−SOURCE VOLTAGE (VOLTS)  
V , GATE−TO−SOURCE VOLTAGE (VOLTS)  
GS  
Figure 1. OnRegion Characteristics  
Figure 2. Transfer Characteristics  
0.26  
0.22  
0.18  
0.14  
0.1  
0.6  
0.5  
0.4  
0.3  
V
GS  
= 10 V  
T = 25°C  
J
V
GS  
= 10 V  
T = 100°C  
J
15 V  
25°C  
0.2  
0.1  
0
55°C  
0
5
10  
15  
20  
25  
30  
35  
0
8
16  
24  
32  
I , DRAIN CURRENT (AMPS)  
D
I , DRAIN CURRENT (AMPS)  
D
Figure 3. OnResistance versus Drain Current  
Figure 4. OnResistance versus Drain Current  
and Temperature  
and Gate Voltage  
1000  
100  
10  
3.0  
2.5  
2.0  
1.5  
1.0  
0.5  
0
V
GS  
= 0 V  
V
GS  
I = 8 A  
= 10 V  
T = 125°C  
D
J
100°C  
25°C  
1
−50  
−25  
0
25  
50  
75  
100  
125  
150  
0
50  
V
100  
150  
200  
250  
3
T , JUNCTION TEMPERATURE (°C)  
J
, DRAIN−TO−SOURCE VOLTAGE (VOLTS)  
DS  
Figure 5. OnResistance Variation with  
Figure 6. DrainToSource Leakage  
Temperature  
Current versus Voltage  
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MTB16N25E  
POWER MOSFET SWITCHING  
The capacitance (Ciss) is read from the capacitance curve  
at a voltage corresponding to the offstate condition when  
calculating td(on) and is read at a voltage corresponding to  
Switching behavior is most easily modeled and predicted  
by recognizing that the power MOSFET is charge  
controlled. The lengths of various switching intervals (Δt)  
are determined by how fast the FET input capacitance can  
be charged by current from the generator.  
the onstate 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 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.  
The published capacitance data is difficult to use for  
calculating rise and fall because draingate 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 as 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 turnon and turnoff 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  
)
5000  
4000  
V
GS  
= 0 V  
V
DS  
= 0 V  
T = 25°C  
J
C
iss  
3000  
2000  
C
iss  
C
rss  
1000  
0
C
oss  
C
rss  
10  
5
0
5
10  
15  
20  
25  
V
GS  
V
DS  
GATE−TO−SOURCE OR DRAIN−TO−SOURCE VOLTAGE (VOLTS)  
Figure 7. Capacitance Variation  
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MTB16N25E  
12  
9
1000  
200  
150  
100  
QT  
V
DD  
I = 16 A  
= 250 V  
D
V
GS  
V
GS  
= 10 V  
T = 25°C  
J
100  
t
r
Q1  
Q2  
t
f
t
t
d(off)  
6
3
0
d(on)  
10  
1
I = 16 A  
D
T = 25°C  
J
50  
0
Q3  
10  
V
DS  
1
10  
R , GATE RESISTANCE (OHMS)  
1
0
20  
30  
40  
50  
60  
Q , TOTAL CHARGE (nC)  
T
G
Figure 8. GateToSource and DrainToSource  
Figure 9. Resistive Switching Time  
Variation versus Gate Resistance  
Voltage versus Total Charge  
DRAINTOSOURCE DIODE CHARACTERISTICS  
16  
V
GS  
= 0 V  
T = 25°C  
J
12  
8
4
0
0.5  
0.55 0.6  
0.65 0.7  
0.75 0.8  
0.85 0.9 0.95  
V
SD  
, SOURCE−TO−DRAIN VOLTAGE (VOLTS)  
Figure 10. Diode Forward Voltage versus Current  
SAFE OPERATING AREA  
A Power MOSFET designated EFET can be safely used  
The Forward Biased Safe Operating Area curves define  
the maximum simultaneous draintosource 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  
ResistanceGeneral Data and Its Use.”  
in switching circuits with unclamped inductive loads. For  
reliable 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 nonlinearly with  
an increase of peak current in avalanche and peak junction  
temperature.  
Switching between the offstate and the onstate 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).  
Although many EFETs can withstand the stress of  
draintosource 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 must be derated for temperature as  
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6
MTB16N25E  
shown in the accompanying graph (Figure 12). Maximum  
energy at currents below rated continuous ID can safely be  
assumed to equal the values indicated.  
SAFE OPERATING AREA  
100  
10  
1
400  
V
= 20 V  
SINGLE PULSE  
GS  
I = 16 A  
D
10ꢀμs  
T = 25°C  
C
300  
200  
100  
0
100ꢀμs  
1ꢀms  
10ꢀms  
dc  
R
LIMIT  
DS(on)  
THERMAL LIMIT  
PACKAGE LIMIT  
0.1  
0.1  
1.0  
10  
100  
1000  
25  
50  
75  
100  
125  
1
V
DS  
, DRAIN−TO−SOURCE VOLTAGE (VOLTS)  
T , STARTING JUNCTION TEMPERATURE (°C)  
J
Figure 11. Maximum Rated Forward Biased  
Safe Operating Area  
Figure 12. Maximum Avalanche Energy versus  
Starting Junction Temperature  
1.0  
D = 0.5  
0.2  
0.1  
0.1  
0.05  
0.02  
P
(pk)  
R
θ
(t) = r(t) R  
θ
JC  
JC  
D CURVES APPLY FOR POWER  
PULSE TRAIN SHOWN  
READ TIME AT t  
t
1
0.01  
1
t
2
T
− T = P  
C
R (t)  
θ
JC  
J(pk)  
(pk)  
DUTY CYCLE, D = t /t  
SINGLE PULSE  
1 2  
0.01  
0.00001  
0.0001  
0.001  
0.01  
0.1  
1.0  
10  
t, TIME (s)  
Figure 13. Thermal Response  
3
R
= 50°C/W  
θ
JA  
Board material = 0.065 mil FR4  
Mounted on the minimum recommended footprint  
Collector/Drain Pad Size 9 450 mils x 350 mils  
2.5  
2.0  
1.5  
1
di/dt  
I
S
t
rr  
t
a
t
b
TIME  
0.5  
0.25 I  
t
p
S
0
25  
50  
75  
100  
125  
15  
I
S
T , AMBIENT TEMPERATURE (°C)  
A
Figure 14. Diode Reverse Recovery Waveform  
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Figure 15. D2PAK Power Derating Curve  
7
MTB16N25E  
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.  
0.33  
8.38  
0.08  
2.032  
0.24  
0.42  
10.66  
6.096  
0.04  
1.016  
0.12  
3.05  
0.63  
17.02  
inches  
mm  
POWER DISSIPATION FOR A SURFACE MOUNT DEVICE  
The power dissipation for a surface mount device is a  
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 RθJA versus drain pad area is shown in  
Figure 16.  
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 TJ(max), the maximum rated  
junction temperature of the die, RθJA, 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:  
70  
Board Material = 0.0625″  
G−10/FR−4, 2 oz Copper  
T = 25°C  
A
60  
2.5 Watts  
TJ(max) TA  
PD =  
50  
Rθ  
JA  
3.5 Watts  
40  
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.  
5 Watts  
30  
20  
0
2
4
6
8
10  
12  
14  
16  
150°C 25°C  
A, AREA (SQUARE INCHES)  
= 2.5 Watts  
PD =  
50°C/W  
Figure 16. Thermal Resistance versus Drain Pad  
Area for the D2PAK Package (Typical)  
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  
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.  
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MTB16N25E  
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  
SC59, SC70/SOT323, SOD123, SOT23, SOT143,  
SOT223, SO8, SO14, SO16, 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.  
SOLDER PASTE  
OPENINGS  
STENCIL  
Figure 17. Typical Stencil for DPAK and  
D2PAK Packages  
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 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.  
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.  
* 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.  
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MTB16N25E  
TYPICAL SOLDER HEATING PROFILE  
For any given circuit board, there will be a group of control  
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 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 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  
STEP 1  
PREHEAT  
ZONE 1  
ꢁRAMP"  
STEP 2  
VENT  
STEP 3  
HEATING  
STEP 4  
HEATING  
STEP 5  
HEATING  
STEP 6  
VENT  
STEP 7  
COOLING  
ꢁSOAK" ZONES 2 & 5  
ꢁRAMP"  
ZONES 3 & 6 ZONES 4 & 7  
ꢁSOAK" ꢁSPIKE"  
170°C  
205° TO 219°C  
PEAK AT  
SOLDER JOINT  
200°C  
150°C  
100°C  
50°C  
DESIRED CURVE FOR HIGH  
MASS ASSEMBLIES  
160°C  
150°C  
SOLDER IS LIQUID FOR  
40 TO 80 SECONDS  
(DEPENDING ON  
100°C  
140°C  
MASS OF ASSEMBLY)  
DESIRED CURVE FOR LOW  
MASS ASSEMBLIES  
TIME (3 TO 7 MINUTES TOTAL)  
T
MAX  
Figure 18. Typical Solder Heating Profile  
http://onsemi.com  
10  
MTB16N25E  
PACKAGE DIMENSIONS  
CASE 418B02  
ISSUE B  
C
E
V
B
NOTES:  
1. DIMENSIONING AND TOLERANCING PER ANSI  
Y14.5M, 1982.  
4
2. CONTROLLING DIMENSION: INCH.  
INCHES  
DIM MIN MAX  
MILLIMETERS  
STYLE 2:  
PIN 1. GATE  
A
MIN  
8.64  
9.65  
4.06  
0.51  
1.14  
MAX  
9.65  
10.29  
4.83  
0.89  
1.40  
S
A
B
C
D
E
G
H
J
0.340  
0.380  
0.160  
0.020  
0.045  
0.380  
0.405  
0.190  
0.035  
0.055  
2. DRAIN  
3. SOURCE  
4. DRAIN  
1
2
3
T−  
SEATING  
PLANE  
K
0.100 BSC  
2.54 BSC  
0.080  
0.018  
0.090  
0.575  
0.045  
0.110  
0.025  
0.110  
0.625  
0.055  
2.03  
0.46  
2.79  
0.64  
J
G
K
S
V
2.29  
14.60  
1.14  
2.79  
15.88  
1.40  
H
D 3 PL  
M
0.13 (0.005)  
T
ON Semiconductor and  
are registered trademarks of Semiconductor Components Industries, LLC (SCILLC). SCILLC reserves the right to make changes without further notice  
to any products herein. SCILLC makes no warranty, representation or guarantee regarding the suitability of its products for any particular purpose, nor does SCILLC assume any liability  
arising out of the application or use of any product or circuit, and specifically disclaims any and all liability, including without limitation special, consequential or incidental damages.  
“Typical” parameters which may be provided in SCILLC data sheets and/or specifications can and do vary in different applications and actual performance may vary over time. All  
operating parameters, including “Typicals” must be validated for each customer application by customer’s technical experts. SCILLC does not convey any license under its patent rights  
nor the rights of others. SCILLC 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 SCILLC product could create a situation where personal injury or death may occur. Should  
Buyer purchase or use SCILLC products for any such unintended or unauthorized application, Buyer shall indemnify and hold SCILLC 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 SCILLC was negligent regarding the design or manufacture of the part. SCILLC is an Equal  
Opportunity/Affirmative Action Employer. This literature is subject to all applicable copyright laws and is not for resale in any manner.  
PUBLICATION ORDERING INFORMATION  
LITERATURE FULFILLMENT:  
N. American Technical Support: 8002829855 Toll Free  
USA/Canada  
Europe, Middle East and Africa Technical Support:  
Phone: 421 33 790 2910  
Japan Customer Focus Center  
Phone: 81357733850  
ON Semiconductor Website: www.onsemi.com  
Order Literature: http://www.onsemi.com/orderlit  
Literature Distribution Center for ON Semiconductor  
P.O. Box 5163, Denver, Colorado 80217 USA  
Phone: 3036752175 or 8003443860 Toll Free USA/Canada  
Fax: 3036752176 or 8003443867 Toll Free USA/Canada  
Email: orderlit@onsemi.com  
For additional information, please contact your local  
Sales Representative  
MTB16N25E/D  

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