Datasheet MTP50P03HDL Datasheet (Motorola)

Page 1
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SEMICONDUCTOR TECHNICAL DATA
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P–Channel Enhancement–Mode Silicon Gate
Avalanche Energy Specified
Source–to–Drain Diode Recovery Time Comparable to a Dis-
crete Fast Recovery Diode
Diode is Characterized for Use in Bridge Circuits
I
MAXIMUM RATINGS
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.
Designer’s, E–FET and HDTMOS are trademarks of Motorola, Inc. TMOS is a registered trademark of Motorola, Inc.
and V
DSS
Drain–Source Voltage V Drain–Gate Voltage (RGS = 1.0 M) V Gate–Source Voltage — Continuous
— Non–Repetitive (tp 10 ms) Drain Current — Continuous
Drain Current — Continuous @ 100°C Drain Current — Single Pulse (tp 10 µs)
Total Power Dissipation
Derate above 25°C Operating and Storage Temperature Range TJ, T Single Pulse Drain–to–Source Avalanche Energy — Starting TJ = 25°C
(VDD = 25 Vdc, VGS = 5.0 Vdc, Peak IL = 50 Apk, L = 1.0 mH, RG = 25 Ω) Thermal Resistance — Junction to Case
Thermal Resistance — Junction to Ambient, when mounted with the minimum recommended pad size
Maximum Lead Temperature for Soldering Purposes, 1/8 from case for 10 seconds T
Specified at Elevated Temperature
DS(on)
(TC = 25°C unless otherwise noted)
D
G
S
Rating
TMOS POWER FET
LOGIC LEVEL
50 AMPERES
30 VOLTS
R
CASE 221A–06, Style 5
Symbol Value Unit
DSS
DGR
V
GS
V
GSM
I
D
I
D
I
DM P
D
E
AS
R
θJC
R
θJA
L
= 0.025 OHM
DS(on)
TO–220AB
± 15 ± 20
150 125
–55 to 150 °C
stg
1250 mJ
62.5 260 °C
30 Vdc 30 Vdc
Vdc Vpk
50 31
1.0
1.0
Adc
Apk
Watts
W/°C
°C/W
Preferred devices are Motorola recommended choices for future use and best overall value.
REV 2
Motorola TMOS Power MOSFET Transistor Device Data
Motorola, Inc. 1997
1
Page 2
MTP50P03HDL
)
f = 1.0 MHz)
V
RG 2.3 )
(
DS
,
D
,
(
S
,
GS
,
ELECTRICAL CHARACTERISTICS
OFF CHARACTERISTICS
Drain–to–Source Breakdown Voltage (Cpk 2.0) (3)
(VGS = 0 Vdc, ID = 250 µAdc) T emperature Coef ficient (Positive)
Zero Gate Voltage Drain Current
(VDS = 30 Vdc, VGS = 0 Vdc) (VDS = 30 Vdc, VGS = 0 Vdc, TJ = 125°C)
Gate–Body Leakage Current
(VGS = ± 15 Vdc, VDS = 0 Vdc)
ON CHARACTERISTICS (1)
Gate Threshold Voltage (Cpk 3.0) (3)
(VDS = VGS, ID = 250 µAdc) Threshold Temperature Coefficient (Negative)
Static Drain–to–Source On–Resistance (Cpk 3.0) (3)
(VGS = 5.0 Vdc, ID = 25 Adc)
Drain–to–Source On–Voltage (VGS = 10 Vdc)
(ID = 50 Adc) (ID = 25 Adc, TJ = 125°C)
Forward Transconductance
(VDS = 5.0 Vdc, ID = 25 Adc)
DYNAMIC CHARACTERISTICS
Input Capacitance Output Capacitance Transfer Capacitance
SWITCHING CHARACTERISTICS (2)
Turn–On Delay Time Rise Time Turn–Off Delay Time Fall Time Gate Charge
(See Figure 8)
SOURCE–DRAIN DIODE CHARACTERISTICS
Forward On–Voltage
Reverse Recovery Time
(See Figure 15)
Reverse Recovery Stored Charge Q
INTERNAL PACKAGE INDUCTANCE
Internal Drain Inductance
(Measured from contact screw on tab to center of die) (Measured from the drain lead 0.25 from package to center of die)
Internal Source Inductance
(Measured from the source lead 0.25 from package to source bond pad)
(1) Pulse Test: Pulse Width 300 µs, Duty Cycle 2%. (2) Switching characteristics are independent of operating junction temperature. (3) Reflects typical values.
Cpk =
(TJ = 25°C unless otherwise noted)
Characteristic Symbol Min Typ Max Unit
(VDS = 25 Vdc, VGS = 0 Vdc,
(IS = 50 Adc, VGS = 0 Vdc, TJ = 125°C)
Max limit – Typ
3 x SIGMA
f = 1.0 MHz
(VDD = 15 Vdc, ID = 50 Adc,
(VDS = 24 Vdc, ID = 50 Adc,
(IS =50 Adc, VGS = 0 Vdc)
(IS = 50 Adc, VGS = 0 Vdc,
= 5.0 Vdc,
GS RG = 2.3 )
VGS = 5.0 Vdc)
dIS/dt = 100 A/µs)
V
(BR)DSS
I
DSS
I
GSS
V
GS(th)
R
DS(on)
V
DS(on)
g
FS
C
iss
C
oss
C
rss
t
d(on)
t
r
t
d(off)
t
f
Q Q Q Q
V
SD
t
rr
t
a
t
b
RR
L
D
L
S
30 —
— —
100
1.0 —
0.020 0.025
— —
15 20
3500 4900 pF — 1550 2170 — 550 770
22 30 ns — 340 466 — 90 117 — 218 300
T 1 2 3
74 100 nC — 13.6 — — 44.8 — — 35
— —
106 — — 58 — — 48 — — 0.246 µ C
— —
7.5
— 26
— —
1.5
4.0
0.83 —
2.39
1.84
3.5
4.5
— —
1.0 10
2.0 —
1.5
1.3
3.0 —
— —
Vdc
mV/°C
µAdc
nAdc
Vdc
mV/°C
Ohm
Vdc
mhos
Vdc
ns
nH
nH
2
Motorola TMOS Power MOSFET Transistor Device Data
Page 3
TYPICAL ELECTRICAL CHARACTERISTICS
MTP50P03HDL
100
TJ = 25°C
80
60
40
, DRAIN CURRENT (AMPS)
D
I
20
0
0 0.4 0.8 1.2 1.6 2.00.2 0.6 1.0 1.4 1.8
VDS, DRAIN–TO–SOURCE VOL TAGE (VOLTS) VGS, GATE–T O–SOURCE VOLT AGE (VOLTS)
VGS = 10 V
8 V
6 V
Figure 1. On–Region Characteristics Figure 2. Transfer Characteristics
0.029 V
= 5.0 V
GS
0.027
0.025
0.023
0.021
TJ = 100°C
25°C
5 V
4.5 V
4 V
3.5 V
3 V
2.5 V
100
VDS ≥ 10 V
80
60
40
, DRAIN CURRENT (AMPS)
D
I
20
0
1.5 1.9 2.3 2.7 3.5 4.33.1 3.9
0.022 TJ = 25°C
0.021
0.020
0.019
0.018
VGS = 5 V
TJ = – 55°C
25°C
100°C
0.019
, DRAIN–TO–SOURCE RESIST ANCE (OHMS)
0.017
DS(on)
0.015
R
020406080100
ID, DRAIN CURRENT (AMPS)
–55°C
Figure 3. On–Resistance versus Drain Current
and T emperature
1.35 VGS = 5 V ID = 25 A
1.25
1.15
1.05
(NORMALIZED)
, DRAIN–TO–SOURCE RESIST ANCE
0.95
DS(on)
R
0.85
– 50 – 25 0 25 50 75 100 125 150
TJ, JUNCTION TEMPERATURE (
°
C)
0.017
, DRAIN–TO–SOURCE RESIST ANCE (OHMS)
0.016
0.015
DS(on)
R
020406080100
ID, DRAIN CURRENT (AMPS)
10 V
Figure 4. On–Resistance versus Drain Current
and Gate Voltage
1000
VGS = 0 V
TJ = 125°C
100
, LEAKAGE (nA)
DSS
I
100°C
10
0 5 10 20 25 30
VDS, DRAIN–TO–SOURCE VOL TAGE (VOLTS)
15
Figure 5. On–Resistance Variation with
Temperature
Motorola TMOS Power MOSFET Transistor Device Data
Figure 6. Drain–T o–Source Leakage
Current versus Voltage
3
Page 4
MTP50P03HDL
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 rudimentary analysis of
G(A V)
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 times may
SGP
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/(VGG – V
iss
In (VGG/V
iss
GSP
)]
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.
14000
VDS = 0 V
12000
C
10000
C, CAPACITANCE (pF)
iss
8000
6000
C
rss
4000
2000
0
10 0 10 15 20 25
55
GATE–T O–SOURCE OR DRAIN–TO–SOURCE VOLTAGE (VOLTS)
VGS = 0 V
C
rss
V
GS
V
DS
T
C
iss
C
oss
Figure 7. Capacitance Variation
= 25°C
J
4
Motorola TMOS Power MOSFET Transistor Device Data
Page 5
6 30
QT
5
Q1
4
3
Q2
V
GS
25
20
15
1000
VDD = 30 V ID = 50 A VGS = 10 V TJ = 25
100
MTP50P03HDL
°
C
t
d(off)
t
r
t
f
2
, GATE–T O–SOURCE VOLT AGE (VOLTS)
1
GS
V
0
010 40 60708030 50
Q3
20
QT, TOTAL GATE CHARGE (nC) RG, GATE RESISTANCE (Ohms)
ID = 50 A TJ = 25
V
DS
10
°
C
5
0
Figure 8. Gate–T o–Source and Drain–To–Source
V oltage versus Total Charge
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
t, TIME (ns)
t
, DRAIN–TO–SOURCE VOL TAGE (VOLTS)
DS
V
10
110
d(on)
Figure 9. Resistive Switching Time
Variation versus Gate Resistance
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 Motorola 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.
50
VGS = 0 V TJ = 25
°
C
40
30
20
, SOURCE CURRENT (AMPS)
S
I
10
0
0.4 0.8 1.2 1.6 2.0 2.4
0.6 1.0 1.4 1.8 2.2 VSD, SOURCE–TO–DRAIN VOL TAGE (VOLTS)
Figure 10. Diode Forward V oltage versus Current
Motorola TMOS Power MOSFET Transistor Device Data
5
Page 6
MTP50P03HDL
di/dt = 300 A/µs
, SOURCE CURRENT
S
I
Figure 11. Reverse Recovery T ime (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 (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 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 (IDM) nor rated voltage (V 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
A power MOSFET designated E–FET can be safely used in switching circuits with unclamped inductive loads. For reli-
) is exceeded, and that the transition
DSS
).
θJC
Standard Cell Density
t
rr
High Cell Density
t
rr
t
b
t
a
t, TIME
able 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 (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 shown in the accompanying graph (Figure 13). Maximum energy at cur­rents below rated continuous ID can safely be assumed to equal the values indicated.
1000
VGS = 20 V SINGLE PULSE
°
C
TC = 25
100
10
, DRAIN CURRENT (AMPS)
D
I
1
0.1 1.0 10 100 VDS, DRAIN–TO–SOURCE VOL TAGE (VOLTS) TJ, STARTING JUNCTION TEMPERATURE (°C)
R
LIMIT
DS(on)
THERMAL LIMIT PACKAGE LIMIT
100 µs
1 ms 10 ms
dc
Figure 12. Maximum Rated Forward Biased
Safe Operating Area
6
1400
1200
1000
800
600
400
AVALANCHE ENERGY (mJ)
, SINGLE PULSE DRAIN–TO–SOURCE
200
AS
E
0
25 15050 100 12575
ID = 50 A
Figure 13. Maximum Avalanche Energy versus
Starting Junction T emperature
Motorola TMOS Power MOSFET Transistor Device Data
Page 7
1.0
MTP50P03HDL
D = 0.5
0.2
0.1
0.1
0.05
0.02
(NORMALIZED)
0.01
SINGLE PULSE
0.01
1.0E–05 1.0E–04 1.0E–021.0E–03
r(t), EFFECTIVE TRANSIENT THERMAL RESISTANCE
t, TIME (s)
Figure 14. Thermal Response
di/dt
I
S
t
a
t
p
P
(pk)
t
1
DUTY CYCLE, D = t1/t
t
rr
t
b
0.25 I
S
I
S
t
2
0.1
1.0E–01
TIME
R
(t) = r(t) R
θ
JC
D CURVES APPLY FOR POWER PULSE TRAIN SHOWN READ TIME AT t T
J(pk)
2
θ
JC
– TC = P
1
R
(pk)
1.0E+00 1.0E+01
(t)
θ
JC
Figure 15. Diode Reverse Recovery Waveform
Motorola TMOS Power MOSFET Transistor Device Data
7
Page 8
MTP50P03HDL
P ACKAGE DIMENSIONS
SEATING
–T–
PLANE
B
4
Q
123
F
T
A
U
H
K
Z
L
V
C
S
STYLE 5:
PIN 1. GATE
2. DRAIN
3. SOURCE
4. DRAIN
R J
G
D
N
CASE 221A–06
NOTES:
1. DIMENSIONING AND TOLERANCING PER ANSI Y14.5M, 1982.
2. CONTROLLING DIMENSION: INCH.
3. DIMENSION Z DEFINES A ZONE WHERE ALL BODY AND LEAD IRREGULARITIES ARE ALLOWED.
DIM MIN MAX MIN MAX
A 0.570 0.620 14.48 15.75 B 0.380 0.405 9.66 10.28 C 0.160 0.190 4.07 4.82 D 0.025 0.035 0.64 0.88 F 0.142 0.147 3.61 3.73 G 0.095 0.105 2.42 2.66 H 0.110 0.155 2.80 3.93 J 0.018 0.025 0.46 0.64 K 0.500 0.562 12.70 14.27 L 0.045 0.060 1.15 1.52 N 0.190 0.210 4.83 5.33 Q 0.100 0.120 2.54 3.04 R 0.080 0.110 2.04 2.79 S 0.045 0.055 1.15 1.39 T 0.235 0.255 5.97 6.47 U 0.000 0.050 0.00 1.27 V 0.045 ––– 1.15 ––– Z ––– 0.080 ––– 2.04
MILLIMETERSINCHES
ISSUE Y
Motorola reserves the right to make changes without further notice to any products herein. Motorola makes no warranty , representation or guarantee regarding the suitability of its products for any particular purpose, nor does Motorola 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 consequential or incidental damages. “T ypical” parameters which may be provided in Motorola 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. Motorola does not convey any license under its patent rights nor the rights of others. Motorola 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 Motorola product could create a situation where personal injury or death may occur. Should Buyer purchase or use Motorola products for any such unintended or unauthorized application, Buyer shall indemnify and hold Motorola 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 Motorola was negligent regarding the design or manufacture of the part. Motorola and are registered trademarks of Motorola, Inc. Motorola, Inc. is an Equal Opportunity/Affirmative Action Employer.
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Motorola TMOS Power MOSFET Transistor Device Data
Mfax is a trademark of Motorola, Inc.
MTP50P03HDL/D
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