Datasheet NTMS7N03R2 Datasheet (ON Semiconductor)

Page 1
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NTMS7N03R2
Power MOSFET 7 Amps, 30 Volts
Features
Ultra Low R
Higher Efficiency Extending Battery Life
Logic Level Gate Drive
Miniature SO-8 Surface Mount Package
Avalanche Energy Specified
I
Specified at Elevated Temperature
DSS
T ypical Applications
DC-DC Converters
Power Management
Motor Controls
Inductive Loads
Replaces MMSF7N03HD, MMSF7N03Z, and MMSF5N03HD in
Many Applications
DS(on)
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7 AMPERES
30 VOLTS
= 23 m
N-Channel
D
G
R
DS(on)
MAXIMUM RATINGS (T
Rating Symbol Value Unit
Drain-to-Source Voltage V Drain-to-Gate Voltage (RGS = 1.0 MΩ) V Gate-to-Source Voltage - Continuous V Thermal Resistance - Junction to Ambient
(Note 1) Total Power Dissipation @ TA = 25°C P Drain Current - Continuous @ TA = 25°C
Drain Current - Continuous @ T Drain Current - Pulsed (Note 4)
Thermal Resistance - Junction to Ambient
(Note 2) Total Power Dissipation @ TA = 25°C P Drain Current - Continuous @ TA = 25°C
Drain Current - Continuous @ T Drain Current - Pulsed (Note 4)
Thermal Resistance - Junction to Ambient
(Note 3) Total Power Dissipation @ TA = 25°C P Drain Current - Continuous @ TA = 25°C
Drain Current - Continuous @ T Drain Current - Pulsed (Note 4)
Operating and Storage Temperature Range TJ, T
Single Pulse Drain-to-Source Avalanche
Energy - Starting T
(V
= 30 Vdc, VGS = 10 Vdc, Peak
DD
I
= 12 Apk, L = 4.0 mH, RG = 25 Ω)
L
1. 2 SQ. FR-4 PCB mounting, (2 oz. Cu 0.06 thick single sided), 10 Sec. Max.
2. 2 SQ. FR-4 PCB mounting, (2 oz. Cu 0.06 thick single sided), t = steady state.
3. Minimum FR4 or G10 PCB, t = steady state.
4. Pulse test: Pulse Width = 300 µs, Duty Cycle = 2%.
= 25°C unless otherwise noted)
C
= 70°C
A
= 70°C
A
= 70°C
A
= 25°C
J
R
R
R
E
DSS DGR
GS
θ
I I
I
DM
θ
I I
I
DM
θ
I I
I
DM
AS
30 Vdc 30 Vdc
± 20 Vdc
JA
D
D D
JA
D
D D
JA
D
D D
stg
50 °C/W
2.5 Watts
8.5
6.8 25
85 °C/W
1.47 Watts
6.5
5.2 18
156 °C/W
0.8 Watts
4.8
3.8 14
- 55 to +150
288 mJ
Adc
Apk
Adc
Apk
Adc
Apk
°C
S
MARKING DIAGRAM
SO-8
8
1
CASE 751 STYLE 13
E7N03 = Device Code A = Assembly Location Y = Year WW = Work Week
E7N03 AYWW
PIN ASSIGNMENT
N-C Source Source
Gate
1 2 3 4
Top View
Drain
8
Drain
7
Drain
6 5
Drain
ORDERING INFORMATION
Device Package Shipping
NTMS7N03R2 SO-8 2500/Tape & Reel
Semiconductor Components Industries, LLC, 2002
November, 2002 - Rev. 3
1
Publication Order Number:
NTMS7N03R2/D
Page 2
NTMS7N03R2
)
f = 1.0 MHz)
R
G
9.1 ) (Note 5)
R
G
9.1 ) (Note 5)
(V
DS
Vdc, I
D
Adc
(I
S
Adc, V
GS
Vdc
ELECTRICAL CHARACTERISTICS (T
= 25°C unless otherwise noted)
C
Characteristic Symbol Min Typ Max Unit
OFF CHARACTERISTICS
Drain-to-Source Breakdown Voltage (Notes 5 and 7)
= 0 Vdc, ID = 0.25 mAdc)
(V
GS
Temperature Coefficient (Positive)
Zero Gate Voltage Drain Current
(V
= 30 Vdc, VGS = 0 Vdc)
DS
= 30 Vdc, VGS = 0 Vdc, TJ = 125°C)
(V
DS
Gate-Body Leakage Current (VGS = ± 20 Vdc, VDS = 0) I
ON CHARACTERISTICS
Gate Threshold Voltage (Note 5)
= VGS, ID = 0.25 mAdc)
(V
DS
Threshold Temperature Coefficient (Negative)
Static Drain-to-Source On-Resistance (Notes 5 and 7)
(V
= 10 Vdc, ID = 7.0 Adc)
GS
(V
= 4.5 Vdc, ID = 3.5 Adc)
GS
Drain-to-Source On-Voltage (VGS = 10 Vdc, ID = 5.0 Adc) (Notes 5 and 7) V Forward Transconductance (VDS = 15 Vdc, ID = 2.0 Adc) (Note 5) g
DYNAMIC CHARACTERISTICS
Input Capacitance Output Capacitance
(VDS = 25 Vdc, VGS = 0 Vdc,
f = 1.0 MHz
Transfer Capacitance
SWITCHING CHARACTERISTICS (Note 6)
Turn-On Delay Time
(V
= 10 Vdc, ID = 5.0 Adc,
Rise Time Turn-Off Delay Time
DD
VGS = 4.5 Vdc,
= 9.1 ) (Note 5)
R
G
Fall Time Turn-On Delay Time t
(V
= 10 Vdc, ID = 5.0 Adc,
Rise Time Turn-Off Delay Time
DD
VGS = 10 Vdc, = 9.1 ) (Note 5)
R
G
Fall Time Gate Charge
(VDS = 16 Vdc, ID = 5.0 Adc,
16
V
= 10 Vdc) (Note 5)
GS
5.0
,
SOURCE-DRAIN DIODE CHARACTERISTICS
Forward On-Voltage (Note 5)
(IS = 7.0 Adc, VGS = 0 Vdc) (Note 5)
= 7.0 Adc, VGS = 0 Vdc,
(I
S
= 125°C)
T
J
Reverse Recovery Time
(IS = 7.0 Adc, VGS = 0 Vdc,
7.0
dI
/dt = 100 A/µs) (Note 5)
S
0
,
Reverse Recovery Stored Charge Q
5. Pulse Test: Pulse Width ≤300 µs, Duty Cycle ≤ 2%.
6. Switching characteristics are independent of operating junction temperature.
7. Reflects Typical Values.
Max limit Typ
Cpk
3
V
(BR)DSS
I
DSS
GSS
V
GS(th)
R
DS(on)
DS(on)
C C C
t
d(on)
t
d(off)
d(on)
t
d(off)
Q
Q Q Q
V
t t t
FS
iss oss rss
t
r
t
f
t
r
t
f
SD
rr
a
b RR
30
-
41
-
-
-
mV/°C
µAdc
Vdc
-
-
0.02
-
1.0 10
- - 100 nAdc
Vdc
1.0
-
1.6
4.0
3.0
-
mV/°C
m
-
-
18.6
23.5
23 28
- 93 115 mV
3.0 13 - Mhos
- 1064 1190 pF
- 300 490
- 94 120
- 15 30
ns
- 71 185
- 27 70
- 38 80
- 8.0 -
- 38 -
- 33 -
- 49
T 1 2 3
- 26 43
- 3.1 -
- 6.0 -
- 5.5 -
-
-
0.82
0.67
1.1
-
- 27 -
nC
Vdc
ns
- 15 -
- 11.5 -
- 0.02 - µC
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NTMS7N03R2
ATTRIBUTES
Characteristics Value
ESD Protection Human Body Model
Machine Model Charged Device Model
TYPICAL ELECTRICAL CHARACTERISTICS
Class 1E
Class A Class 0
20 18 16 14 12 10
, DRAIN CURRENT (AMPS)
D
I
VGS = 10 V
8 V
7 V
6 V
5 V
8 6 4 2
0
0 0.1 0.2 0.3 1
V
, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
DS
0.4 0.5
3.6 V
3.8 V
4 V
4.6 V
TJ = 25°C
2.4 V
0.8 0.9
Figure 1. On-Region Characteristics
3.4 V
3.2 V
3 V
2.8 V
10
9
VDS = 10 V 8 7
6 5 4 3
, DRAIN CURRENT (AMPS)
2
D
I
1 0
0 0.5 1 3.5
VGS, GATE-TO-SOURCE VOLTAGE (VOLTS)
TJ = 100°C
1.50.6 0.7 2
-55°C
2.5 3
Figure 2. Transfer Characteristics
25°C
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NTMS7N03R2
TYPICAL ELECTRICAL CHARACTERISTICS
0.6
0.5
0.4
0.3
0.2
0.1
0
, DRAIN-TO-SOURCE RESISTANCE (OHMS)
13 957
DS(on)
R
24 10
, GATE-TO-SOURCE VOLTAGE (VOLTS)
V
GS
Figure 3. On-Resistance versus
68
Gate-T o-Source Voltage
2
VGS = 10 V
= 3.5 A
I
D
1.5
ID = 3.5 A T
= 25°C
J
0.05 TJ = 25°C
0.04
0.03
VGS = 4.5 V
0.02
0.01
0
, DRAIN-TO-SOURCE RESISTANCE (OHMS)
0 5 10 15
DS(on)
R
Figure 4. On-Resistance versus Drain Current
ID, DRAIN CURRENT (AMPS)
10 V
and Gate Voltage
1000
VGS = 0 V
TJ = 125°C
100
1
(NORMALIZED)
0.5
, DRAIN-TO-SOURCE RESISTANCE
DS(on)
0
R
-50-250 25 50 75 100 125 150 , JUNCTION TEMPERATURE (°C)
T
J
Figure 5. On-Resistance Variation with
Temperature
TJ = 100°C
, LEAKAGE (nA)
10
DSS
I
1
0102030
VDS, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
Figure 6. Drain-To-Source Leakage
Current versus Voltage
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NTMS7N03R2
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
) can be made from a
G(AV)
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
. Therefore, rise and fall
SGP
times may be approximated by the following: tr = Q2 x RG/(VGG - V tf = Q2 x RG/V
GSP
GSP
)
where VGG = the gate drive voltage, which varies from zero to V
GG
RG = the gate drive resistance and Q2 and V
are read from the gate charge curve.
GSP
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)
t
d(off)
= RG C
= RG C
In [VGG/(V
iss
In (VGG/V
iss
GG
GSP
- V
)
GSP
)]
The capacitance (C
) is read from the capacitance curve at
iss
a voltage corresponding to the off-state condition when calculating t on-state when calculating t
and is read at a voltage corresponding to the
d(on)
.
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 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.
V
2800 2400 2000 1600 1200
C, CAPACITANCE (pF)
GATE-T O-SOURCE OR DRAIN-TO-SOURCE VOLTAGE (VOLTS)
VDS = 0 V
C
iss
C
rss
800 400
0
10 0 10 15 20
55
Figure 7. Capacitance Variation
= 0 V
GS
C
rss
V
V
GS
DS
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TJ = 25°C
C
iss
C
oss
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NTMS7N03R2
10
QT
8
V
GS
6
4
, GATE-TO-SOURCE VOLTAGE (VOLTS)
GS
V
Q1
2
0
0
Q2
510 30
, TOTAL GATE CHARGE (nC)
Q
G
15
ID = 3.5 A T
= 25°C
J
20 25
Figure 8. Gate-To-Source and Drain-To-Source
Voltage versus Total Charge
DRAIN-T O-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, t to the storage of minority carrier charge, Q
, as shown in
RR
, due
rr
the typical reverse recovery wave form of Figure 15. 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 t
and low QRR specifications to
rr
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
V
1000
DS
1.2 , DRAIN-TO-SOURCE VOLTAGE (VOLTS)
1.0
0.8
0.6
0.4
0
VDD = 24 V I
= 7 A
D
= 10 V
V
GS
100
t, TIME (ns)
10
1
1 10 100
RG, GATE RESISTANCE (OHMS)
Figure 9. Resistive Switching Time
Variation versus Gate Resistance
high di/dts. The diode’s negative di/dt during t 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 t
serves as a good indicator of recovery
b/ta
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 t
), have less stored charge and a softer
rr
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.
t
d(off)
t
f
t
r
t
d(on)
is directly
a
8 7 6 5 4 3 2
, SOURCE CURRENT (AMPS)
S
1
I
0
0.40 1.00
VGS = 0 V T
= 25°C
J
0.50 0.70
V
SD
0.60 0.80 0.90
, SOURCE-TO-DRAIN VOLTAGE (VOLTS)
Figure 10. Diode Forward Voltage versus Current
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NTMS7N03R2
di/dt = 300 A/µs
, SOURCE CURRENT
S
I
Figure 11. Reverse Recovery Time (trr)
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 (T
) of 25°C.
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 (I
) nor rated voltage (V
DM
) is exceeded, and that the
DSS
transition time (tr, tf) does not exceed 10 µs. In addition the total power averaged over a complete switching cycle must not exceed (T
J(MAX)
- TC)/(R
).
JC
θ
A power MOSFET designated E-FET can be safely used in switching circuits with unclamped inductive loads. For
Standard Cell Density
t
rr
High Cell Density
t
rr
t
b
t
a
t, TIME
reliable operation, the stored energy from circuit inductance dissipated in the transistor while in avalanche must be less than the rated limit and must be 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 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 (I continuous current (I
), the energy rating is specified at rated
DM
), in accordance with industry
D
custom. The energy rating must be derated for temperature as shown in the accompanying graph (Figure 13). Maximum energy at currents below rated continuous I
can safely be
D
assumed to equal the values indicated.
100
10
VGS = 20 V SINGLE PULSE
1
T
= 25°C
C
R
LIMIT
DS(on)
0.1
, DRAIN CURRENT (AMPS)
D
I
Mounted on 2 sq. FR4 board (1 sq. 2 oz. Cu 0.06 thick single sided) with one die operating, 10s max.
0.01
0.1 V
THERMAL LIMIT PACKAGE LIMIT
1
, DRAIN-TO-SOURCE VOLTAGE (VOLTS)
DS
Figure 12. Maximum Rated Forward Biased
Safe Operating Area
10
400 350
300
10 µs 100 µs
1 ms
10 ms
dc
100
250 200 150 100
50
AVALANCHE ENERGY (mJ)
, SINGLE PULSE DRAIN-TO-SOURCE
AS
E
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ID = 12 A
0
25 50 75 100 125
TJ, STARTING JUNCTION TEMPERATURE (°C)
Figure 13. Maximum Avalanche Energy versus
Starting Junction Temperature
150
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NTMS7N03R2
TYPICAL ELECTRICAL CHARACTERISTICS
1
0.1
0.01
THERMAL RESISTANCE
Rthja(t), EFFECTIVE TRANSIENT
0.001
1.0E-05 1.0E-04 1.0E-03 1.0E-02 1.0E-01 1.0E+00 1.0E+01
D = 0.5
0.2
0.1
0.05
0.02
0.01
SINGLE PULSE
Normalized to θja at 10s.
0.0163 0.0652 0.1988 0.6411 0.9502
Chip
72.416 F1.9437 F0.5541 F0.1668 F0.0307 F
Ambient
1.0E+02 1.0E+03
t, TIME (s)
Figure 14. Thermal Response
di/dt
I
S
t
rr
t
t
a
b
TIME
t
p
0.25 I
S
I
S
Figure 15. Diode Reverse Recovery Waveform
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NTMS7N03R2
INFORMATION FOR USING THE SO-8 SURFACE MOUNT PACKAGE
MINIMUM RECOMMENDED FOOTPRINT FOR SURFACE MOUNTED APPLICATIONS
Surface mount board layout is a c ritical p ortion o f t he total design. The footprint for the semiconductor packages must be the correct size to ensure proper solder connection
0.275
7.0
0.024
0.6
SO-8 POWER DISSIPATION
The power dissipation of the SO-8 is a function of the input pad size. This can vary from the minimum pad size for soldering to the pad size given for maximum power dissipation. Power dissipation for a surface mount device is determined by T temperature of the die, R
, the maximum rated junction
J(max)
, the thermal resistance from
JA
θ
the device junction to ambient; and the operating temperature, TA. Using the values provided on the data sheet for the SO-8 package, PD can be calculated as follows:
PD =
J(max)
A
R
θ
JA
- T
T
The values for the equation are found in the maximum ratings table on the data sheet. Substituting these values
interface between the board and the package. With the correct pad geometry, the packages will self-align when subjected to a solder reflow process.
0.060
1.52
0.155
4.0
0.050
1.270
into the equation for an ambient temperature T
inches
mm
of 25°C,
A
one can calculate the power dissipation of the device which in this case is 2.5 Watts.
PD =
150°C - 25°C
50°C/W
= 2.5 Watts
The 50°C/W for the SO- 8 package assumes the
recommended footprint on a glass epoxy printed circuit board to achieve a power dissipation of 2.5 Watts using the footprint shown. Another alternative would be to use a ceramic substrate or an aluminum core board such as Thermal Clad. Using board material such as Thermal Clad, the power dissipation can be doubled using the same footprint.
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.
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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.
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NTMS7N03R2
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. 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 16 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
200°C
150°C
100°C
STEP 1
PREHEAT
ZONE 1 “RAMP”
DESIRED CURVE FOR HIGH
STEP 2
VENT
“SOAK”
MASS ASSEMBLIES
150°C
100°C
HEATING
ZONES 2 & 5
STEP 3
“RAMP”
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 4
HEATING
ZONES 3 & 6
“SOAK”
160°C
140°C
STEP 5
HEATING
ZONES 4 & 7
“SPIKE”
170°C
SOLDER IS LIQUID FOR
40 TO 80 SECONDS
(DEPENDING ON
MASS OF ASSEMBLY)
STEP 6
VENT
STEP 7
COOLING
205° TO 219°C
PEAK AT SOLDER
JOINT
5°C
DESIRED CURVE FOR LOW
MASS ASSEMBLIES
TIME (3 TO 7 MINUTES TOTAL) T
Figure 16. Typical Solder Heating Profile
MAX
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-Z-
-Y-
NTMS7N03R2
PACKAGE DIMENSIONS
SO-8
CASE 751-07
ISSUE AA
NOTES:
-X­A
58
B
1
S
0.25 (0.010)
4
M
M
Y
K
G
C
SEATING PLANE
0.10 (0.004)
H
D
0.25 (0.010) Z
M
Y
SXS
N
X 45
M
J
1. DIMENSIONING AND TOLERANCING PER ANSI Y14.5M, 1982.
2. CONTROLLING DIMENSION: MILLIMETER.
3. DIMENSION A AND B DO NOT INCLUDE MOLD PROTRUSION.
4. MAXIMUM MOLD PROTRUSION 0.15 (0.006) PER SIDE.
5. DIMENSION D DOES NOT INCLUDE DAMBAR PROTRUSION. ALLOWABLE DAMBAR PROTRUSION SHALL BE 0.127 (0.005) TOTAL IN EXCESS OF THE D DIMENSION AT MAXIMUM MATERIAL CONDITION.
6. 751−01 THRU 751−06 ARE OBSOLETE. NEW STANDARD IS 751−07.
MILLIMETERS
DIMAMIN MAX MIN MAX
4.80 5.00 0.189 0.197
B 3.80 4.00 0.150 0.157 C 1.35 1.75 0.053 0.069 D 0.33 0.51 0.013 0.020 G 1.27 BSC 0.050 BSC H 0.10 0.25 0.004 0.010
J 0.19 0.25 0.007 0.010 K 0.40 1.27 0.016 0.050 M 0 8 0 8

N 0.25 0.50 0.010 0.020 S 5.80 6.20 0.228 0.244
STYLE 13:
PIN 1. N.C.
2. SOURCE
3. SOURCE
4. GATE
5. DRAIN
6. DRAIN
7. DRAIN
8. DRAIN
INCHES
http://onsemi.com
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NTMS7N03R2
Thermal Clad is a registered trademark of the Bergquist Company.
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NTMS7N03R2/D
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