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PDF MTB1306 Data sheet ( Hoja de datos )

Número de pieza MTB1306
Descripción Power MOSFET ( Transistor )
Fabricantes ON Semiconductor 
Logotipo ON Semiconductor Logotipo



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MTB1306
Preferred Device
Power MOSFET
75 Amps, 30 Volts, Logic Level
N−Channel D2PAK
This Power MOSFET is designed to withstand high energy in the
avalanche and commutation modes. The energy efficient design also
offers a drain−to−source diode with 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.
Avalanche Energy Specified
Source−to−Drain Diode Recovery Time Comparable to a Discrete
Fast Recovery Diode
Diode is Characterized for Use in Bridge Circuits
IDSS and VDS(on) Specified at Elevated Temperature
Short Heatsink Tab Manufactured − Not Sheared
Specially Designed Leadframe for Maximum Power Dissipation
MAXIMUM RATINGS (TC = 25°C unless otherwise noted)
Rating
Symbol Value
Unit
Drain−to−Source Voltage
Drain−to−Gate Voltage (RGS = 1.0 M)
Gate−to−Source Voltage
− Continuous
− Non−Repetitive (tp 10 ms)
Drain Current
− Continuous
− Continuous @ 100°C
− Single Pulse (tp 10 µs)
Total Power Dissipation
Derate above 25°C
Total Power Dissipation @ TA = 25°C
(Note 1.)
VDSS
VDGR
VGS
VGSM
ID
ID
IDM
PD
30 Vdc
30 Vdc
± 20 Vdc
± 20 Vpk
75 Adc
59
225 Apk
150 Watts
1.2 W/°C
2.5 Watts
Operating and Storage Temperature
Range
TJ, Tstg
−55 to
150
°C
Single Pulse Drain−to−Source Avalanche
Energy − Starting TJ = 25°C
(VDD = 25 Vdc, VGS = 10 Vdc, Peak
IL = 75 Apk, L = 0.1 mH, RG = 25 )
EAS
mJ
280
Thermal Resistance
− Junction−to−Case
− Junction−to−Ambient
− Junction−to−Ambient (Note 1.)
RθJC
RθJA
RθJA
°C/W
0.8
62.5
50
Maximum Lead Temperature for Soldering
Purposes, 1/8from Case for 5.0
seconds
TL
260 °C
1. When surface mounted to an FR4 board using the minimum recommended
pad size.
http://onsemi.com
75 AMPERES
30 VOLTS
RDS(on) = 6.5 m
N−Channel
D
G
S
12
3
4
D2PAK
CASE 418B
STYLE 2
MARKING DIAGRAM
& PIN ASSIGNMENT
4
Drain
MTB1306
YWW
12
Gate Drain
3
Source
MTB1306
Y
WW
= Device Code
= Year
= Work Week
ORDERING INFORMATION
Device
Package
Shipping
MTB1306
MTB1306T4
D2PAK
D2PAK
50 Units/Rail
800/Tape & Reel
Preferred devices are recommended choices for future use
and best overall value.
© Semiconductor Components Industries, LLC, 2000
September, 2004 − Rev.XXX
1
Publication Order Number:
MTB1306/D

1 page




MTB1306 pdf
MTB1306
10 18
7.5
QT
15
VGS 12
5.0 9.0
Q1
2.5
Q3
0
0 10
Q2
6.0
TJ = 25°C
VDS ID = 75 A
20 30 40
QG, TOTAL GATE CHARGE (nC)
50
3.0
0
60
Figure 8. Gate−To−Source and Drain−To−Source
Voltage versus Total Charge
10,000
1000
VDD = 15 V
ID = 75 A
VGS = 5.0 V
TJ = 25°C
tr
100
tf
td(off)
10
1.0
td(on)
10
RG, GATE RESISTANCE (OHMS)
Figure 9. Resistive Switching Time
Variation versus Gate Resistance
100
DRAIN−TO−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, trr, due
to the storage of minority carrier charge, QRR, as shown in
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 trr and low QRR specifications to
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
high di/dts. The diode’s negative di/dt during ta is directly
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 tb/ta serves as a good indicator of recovery
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 trr), have less stored charge and a softer
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.
http://onsemi.com
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