MTP50P03HDLG ON Semiconductor, MTP50P03HDLG Datasheet - Page 4

MOSFET P-CH 30V 50A TO220AB

MTP50P03HDLG

Manufacturer Part Number
MTP50P03HDLG
Description
MOSFET P-CH 30V 50A TO220AB
Manufacturer
ON Semiconductor
Type
Power MOSFETr
Datasheet

Specifications of MTP50P03HDLG

Fet Type
MOSFET P-Channel, Metal Oxide
Fet Feature
Logic Level Gate
Rds On (max) @ Id, Vgs
25 mOhm @ 25A, 5V
Drain To Source Voltage (vdss)
30V
Current - Continuous Drain (id) @ 25° C
50A
Vgs(th) (max) @ Id
2V @ 250µA
Gate Charge (qg) @ Vgs
100nC @ 5V
Input Capacitance (ciss) @ Vds
4900pF @ 25V
Power - Max
125W
Mounting Type
Through Hole
Package / Case
TO-220-3 (Straight Leads)
Configuration
Single
Transistor Polarity
P-Channel
Resistance Drain-source Rds (on)
0.025 Ohm @ 5 V
Forward Transconductance Gfs (max / Min)
20 S
Drain-source Breakdown Voltage
30 V
Gate-source Breakdown Voltage
+/- 15 V
Continuous Drain Current
50 A
Power Dissipation
125000 mW
Maximum Operating Temperature
+ 175 C
Mounting Style
Through Hole
Minimum Operating Temperature
- 55 C
Number Of Elements
1
Polarity
P
Channel Mode
Enhancement
Drain-source On-res
0.025Ohm
Drain-source On-volt
30V
Gate-source Voltage (max)
±15V
Drain Current (max)
50A
Output Power (max)
Not RequiredW
Frequency (max)
Not RequiredMHz
Noise Figure
Not RequireddB
Power Gain
Not RequireddB
Drain Efficiency
Not Required%
Operating Temp Range
-55C to 175C
Operating Temperature Classification
Military
Mounting
Through Hole
Pin Count
3 +Tab
Package Type
TO-220AB
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Other names
MTP50P03HDLGOS

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by recognizing that the power MOSFET is charge
controlled. The lengths of various switching intervals (Dt)
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
rudimentary analysis of the drive circuit so that
t = Q/I
During the rise and fall time interval when switching a
resistive load, V
known as the plateau voltage, V
times may be approximated by the following:
t
t
where
V
R
and Q
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
t
r
f
d(on)
d(off)
GG
G
= Q
= Q
Switching behavior is most easily modeled and predicted
= the gate drive resistance
= the gate drive voltage, which varies from zero to V
= R
2
2
= R
2
G(AV)
x R
x R
and V
G
G
G
G
C
C
/(V
/V
iss
iss
GSP
GSP
GG
In [V
In (V
GS
are read from the gate charge curve.
− V
remains virtually constant at a level
GG
GG
GSP
/(V
/V
)
G(AV)
GSP
GG
)
− V
SGP
) can be made from a
GSP
. Therefore, rise and fall
14000
12000
10000
8000
6000
4000
2000
)]
0
10
GATE−TO−SOURCE OR DRAIN−TO−SOURCE VOLTAGE (VOLTS)
POWER MOSFET SWITCHING
C
V
C
rss
DS
iss
= 0 V
5
Figure 7. Capacitance Variation
V
GS
http://onsemi.com
MTP50P03HDL
GG
0
V
GS
V
DS
4
= 0 V
5
The capacitance (C
a voltage corresponding to the off−state condition when
calculating t
on−state when calculating t
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.
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.
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.
At high switching speeds, parasitic circuit elements
The resistive switching time variation versus gate
C
rss
10
C
C
d(on)
The
oss
iss
15
T
J
and is read at a voltage corresponding to the
= 25°C
MOSFET
iss
20
) is read from the capacitance curve at
d(off)
25
output
.
capacitance
also

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