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What is MTD20P03HDL?

This electronic component, produced by the manufacturer "ON Semiconductor", performs the same function as "Power MOSFET ( Transistor )".


MTD20P03HDL Datasheet PDF - ON Semiconductor

Part Number MTD20P03HDL
Description Power MOSFET ( Transistor )
Manufacturers ON Semiconductor 
Logo ON Semiconductor Logo 


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MTD20P03HDL
Preferred Device
Power MOSFET
20 Amps, 30 Volts, Logic Level
P−Channel DPAK
This Power MOSFET is designed to withstand high energy in the
avalanche and commutation modes. This energy efficient design also
offers a drain−to−source 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.
Features
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
Pb−Free Packages are Available
http://onsemi.com
V(BR)DSS
30 V
RDS(on) TYP
90 mW@5.0 V
ID MAX
20 A
(Note 1)
P−Channel
D
G
MAXIMUM RATINGS (TC = 25°C unless otherwise noted)
Rating
Symbol Value
Unit
Drain−Source Voltage
Drain−Gate Voltage (RGS = 1.0 MW)
Gate−Source Voltage
− Continuous
− Non−Repetitive (tpv10 ms)
Drain Current
− Continuous
− Continuous @ 100°C
− Single Pulse (tpv10 ms)
Total Power Dissipation
Derate above 25°C
Total Power Dissipation @ TC = 25°C (Note 2)
Operating and Storage Temperature Range
VDSS
VDGR
VGS
VGSM
ID
ID
IDM
PD
TJ, Tstg
30 Vdc
30 Vdc
"15
"20
Vdc
Vpk
19
12
57
75
0.6
1.75
−55 to
150
Adc
Apk
W
W/°C
°C
Single Pulse Drain−to−Source Avalanche
Energy − Starting TJ = 25°C
(VDD = 25 Vdc, VGS = 5.0 Vdc,
IL = 19 Apk, L = 1.1 mH, RG = 25 W)
EAS 200 mJ
Thermal Resistance,
Junction−to−Case
Junction−to−Ambient (Note 1)
Junction−to−Ambient (Note 2)
RqJC
RqJA
RqJA
°C/W
1.67
100
71.4
Maximum Lead Temperature for Soldering
Purposes, 1/8from case for 10 seconds
TL 260 °C
Stresses exceeding Maximum Ratings may damage the device. Maximum
Ratings are stress ratings only. Functional operation above the Recommended
Operating Conditions is not implied. Extended exposure to stresses above the
Recommended Operating Conditions may affect device reliability.
1. When surface mounted to an FR−4 board using the minimum recommended
pad size.
2. When surface mounted to an FR−4 board using the 0.5 sq.in. drain pad size.
4
12
3
DPAK
CASE 369C
STYLE 2
S
MARKING DIAGRAMS
1 Gate
2 Drain
3 Source
YWW
20P
03HLG
4
1
2
3
DPAK
CASE 369D
STYLE 2
1 Gate
2 Drain
3 Source
YWW
20P
03HLG
Y
WW
20P03HL
G
= Year
= Work Week
= Device Code
= Pb−Free Package
ORDERING INFORMATION
See detailed ordering and shipping information in the package
dimensions section on page 7 of this data sheet.
Preferred devices are recommended choices for future use
and best overall value.
© Semiconductor Components Industries, LLC, 2006
July, 2006 − Rev. 7
1
Publication Order Number:
MTD20P03HDL/D

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MTD20P03HDL equivalent
MTD20P03HDL
7 35
6
5
Q1
4
QT 30
Q2 25
VGS
20
3 15
2
ID = 19 A
TJ = 25°C
10
1
Q3
5
VDS
00
0 2 4 6 8 10 12 14 16
QG, TOTAL GATE CHARGE (nC)
Figure 8. Gate−To−Source and Drain−To−Source
Voltage versus Total Charge
1000
VDD = 15 V
ID = 19 A
VGS = 5.0 V
TJ = 25°C
tr
100 tf
td(off)
td(on)
10
1
RG, GATE RESISTANCE (OHMS)
Figure 9. Resistive Switching Time
Variation versus Gate Resistance
10
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 12. 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.
20
VGS = 0 V
TJ = 25°C
16
12
8
4
0
0.3 0.7 1.1 1.5 1.9 2.3 2.7 3.1
VSD, SOURCE−TO−DRAIN VOLTAGE (VOLTS)
Figure 10. Diode Forward Voltage versus Current
http://onsemi.com
5


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