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Motorola TMOS Power MOSFET Transistor Device Data
Designer's
TM
Data Sheet
HDTMOS E-FET
.
TM
High Density Power FET
DPAK for Surface Mount
NChannel EnhancementMode Silicon Gate
This advanced HDTMOS power FET is designed to withstand
high energy in the avalanche and commutation modes. This new
energy efficient design also offers a draintosource 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.
Avalanche Energy Specified
SourcetoDrain Diode Recovery Time Comparable to a Dis-
crete Fast Recovery Diode
Diode is Characterized for Use in Bridge Circuits
IDSS and VDS(on) Specified at Elevated Temperature
Surface Mount Package Available in 16 mm, 13inch/2500
Unit Tape & Reel, Add T4 Suffix to Part Number
MAXIMUM RATINGS
(TC = 25
C unless otherwise noted)
Rating
Symbol
Value
Unit
DrainSource Voltage
VDSS
30
Vdc
DrainGate Voltage (RGS = 1.0 M
)
VDGR
30
Vdc
GateSource Voltage -- Continuous
GateSource Voltage
-- NonRepetitive (tp
10 ms)
VGS
VGSM
15
20
Vdc
Vpk
Drain Current -- Continuous
Drain Current
-- Continuous @ 100
C
Drain Current
-- Single Pulse (tp
10
s)
ID
ID
IDM
20
16
60
Adc
Apk
Total Power Dissipation
Derate above 25
C
Total Power Dissipation @ TC = 25
C, when mounted with the minimum recommended pad size
PD
74
0.6
1.75
Watts
W/
C
Operating and Storage Temperature Range
TJ, Tstg
55 to 150
C
Single Pulse DraintoSource Avalanche Energy -- Starting TJ = 25
C
(VDD = 25 Vdc, VGS = 5.0 Vdc, Peak IL = 20 Apk, L = 1.0 mH, RG = 25
)
EAS
200
mJ
Thermal Resistance -- Junction to Case
Thermal Resistance
-- Junction to Ambient
Thermal Resistance
-- Junction to Ambient, when mounted with the minimum recommended pad size
R
JC
R
JA
R
JA
1.67
100
71.4
C/W
Maximum Lead Temperature for Soldering Purposes, 1/8
from case for 10 seconds
TL
260
C
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, EFET, and HDTMOS are trademarks of Motorola, Inc. TMOS is a registered trademark of Motorola, Inc.
Thermal Clad is a trademark of the Bergquist Company.
Preferred devices are Motorola recommended choices for future use and best overall value.
REV 1
Order this document
by MTD20N03HDL/D
MOTOROLA
SEMICONDUCTOR TECHNICAL DATA
Motorola, Inc. 1995
MTD20N03HDL
TMOS POWER FET
LOGIC LEVEL
20 AMPERES
30 VOLTS
RDS(on) = 0.035 OHM
Motorola Preferred Device
TM
D
S
G
CASE 369A13, Style 2
DPAK
MTD20N03HDL
2
Motorola TMOS Power MOSFET Transistor Device Data
ELECTRICAL CHARACTERISTICS
(TJ = 25
C unless otherwise noted)
Characteristic
Symbol
Min
Typ
Max
Unit
OFF CHARACTERISTICS
DraintoSource Breakdown Voltage
(Cpk
2.0) (3)
(VGS = 0 Vdc, ID = 250
Adc)
Temperature Coefficient (Positive)
V(BR)DSS
30
--
--
43
--
--
Vdc
mV/
C
Zero Gate Voltage Drain Current
(VDS = 30 Vdc, VGS = 0 Vdc)
(VDS = 30 Vdc, VGS = 0 Vdc, TJ = 125
C)
IDSS
--
--
--
--
10
100
Adc
GateBody Leakage Current
(VGS =
15 Vdc, VDS = 0 Vdc)
IGSS
--
--
100
nAdc
ON CHARACTERISTICS (1)
Gate Threshold Voltage
(Cpk
2.0) (3)
(VDS = VGS, ID = 250
Adc)
Threshold Temperature Coefficient (Negative)
VGS(th)
1.0
--
1.5
5.0
2.0
--
Vdc
mV/
C
Static DraintoSource OnResistance
(Cpk
2.0) (3)
(VGS = 4.0 Vdc, ID = 10 Adc)
(VGS = 5.0 Vdc, ID = 10 Adc)
RDS(on)
--
0.034
0.030
0.040
0.035
Ohm
DraintoSource OnVoltage (VGS = 5.0 Vdc)
(ID = 20 Adc)
(ID = 10 Adc, TJ = 125
C)
VDS(on)
--
--
0.55
--
0.8
0.7
Vdc
Forward Transconductance
(VDS = 5.0 Vdc, ID = 10 Adc)
gFS
10
13
--
mhos
DYNAMIC CHARACTERISTICS
Input Capacitance
(VDS = 25 Vdc, VGS = 0 Vdc,
f = 1.0 MHz)
Ciss
--
880
1260
pF
Output Capacitance
(VDS = 25 Vdc, VGS = 0 Vdc,
f = 1.0 MHz)
Coss
--
300
420
Transfer Capacitance
f = 1.0 MHz)
Crss
--
80
112
SWITCHING CHARACTERISTICS (2)
TurnOn Delay Time
(VDD = 15 Vdc, ID = 20 Adc,
VGS = 5.0 Vdc,
RG = 9.1
)
td(on)
--
13
15.8
ns
Rise Time
(VDD = 15 Vdc, ID = 20 Adc,
VGS = 5.0 Vdc,
RG = 9.1
)
tr
--
212
238
TurnOff Delay Time
VGS = 5.0 Vdc,
RG = 9.1
)
td(off)
--
37
30
Fall Time
G = 9.1
)
tf
--
84
96
Gate Charge
(See Figure 8)
(VDS = 24 Vdc, ID = 20 Adc,
VGS = 5.0 Vdc)
QT
--
13.4
18.9
nC
(See Figure 8)
(VDS = 24 Vdc, ID = 20 Adc,
VGS = 5.0 Vdc)
Q1
--
3.0
--
(VDS = 24 Vdc, ID = 20 Adc,
VGS = 5.0 Vdc)
Q2
--
7.3
--
Q3
--
6.0
--
SOURCEDRAIN DIODE CHARACTERISTICS
Forward OnVoltage
(Cpk
2.0) (3)
(IS = 20 Adc, VGS = 0 Vdc)
(IS = 20 Adc, VGS = 0 Vdc, TJ = 125
C)
VSD
--
--
0.95
0.87
1.1
--
Vdc
Reverse Recovery Time
(See Figure 15)
(IS = 20 Adc, VGS = 0 Vdc,
dIS/dt = 100 A/
s)
trr
--
33
--
ns
(See Figure 15)
(IS = 20 Adc, VGS = 0 Vdc,
dIS/dt = 100 A/
s)
ta
--
23
--
(IS = 20 Adc, VGS = 0 Vdc,
dIS/dt = 100 A/
s)
tb
--
10
--
Reverse Recovery Stored Charge
QRR
--
33
--
C
INTERNAL PACKAGE INDUCTANCE
Internal Drain Inductance
(Measured from the drain lead 0.25
from package to center of die)
LD
--
4.5
--
nH
Internal Source Inductance
(Measured from the source lead 0.25
from package to source bond pad)
LS
--
7.5
--
nH
(1) Pulse Test: Pulse Width
300
s, Duty Cycle
2%.
(2) Switching characteristics are independent of operating junction temperature.
(3) Reflects typical values. Cpk = Absolute Value of Spec (SpecAVG/3.516
A).
MTD20N03HDL
3
Motorola TMOS Power MOSFET Transistor Device Data
TYPICAL ELECTRICAL CHARACTERISTICS
R
DS(on)
, DRAINT
OSOURCE RESIST
ANCE
(NORMALIZED)
R
DS(on)
, DRAINT
OSOURCE RESIST
ANCE (OHMS)
R
DS(on)
, DRAINT
OSOURCE RESIST
ANCE (OHMS)
I DSS
, LEAKAGE (nA)
VDS, DRAINTOSOURCE VOLTAGE (Volts)
TJ, JUNCTION TEMPERATURE (
C)
ID, DRAIN CURRENT (Amps)
ID, DRAIN CURRENT (Amps)
VDS, DRAINTOSOURCE VOLTAGE (Volts)
VGS, GATETOSOURCE VOLTAGE (Volts)
I D
, DRAIN CURRENT
(AMPS)
I D
, DRAIN CURRENT
(AMPS)
0
0.4
0.8
1.2
1.6
2.0
0.2
0.6
1.0
1.4
1.8
0
10
20
40
Figure 1. OnRegion Characteristics
0
10
20
30
40
Figure 2. Transfer Characteristics
0
16
32
40
0.020
0.028
0.036
0.044
0.052
0.020
0.028
0.036
Figure 3. OnResistance versus Drain Current
and Temperature
Figure 4. OnResistance versus Drain Current
and Gate Voltage
0.6
0.8
1.0
1.2
1.8
1
1000
Figure 5. OnResistance Variation with
Temperature
Figure 6. DrainToSource Leakage
Current versus Voltage
30
VGS = 10 V
8 V
6 V
2.5 V
3 V
TJ = 25
C
4 V
1.0
1.8
2.6
3.4
4.6
4.2
5.0
VDS
10 V
100
C
25
C
VGS = 5 V
55
C
25
C
0
16
24
32
40
0.032
0.024
50
25
0
25
50
75
100
125
150
1.4
0
6
12
24
30
18
VGS = 0 V
TJ = 125
C
TJ = 55
C
TJ = 100
C
TJ = 25
C
VGS = 5 V
10 V
VGS = 5 V
ID = 10 A
1.4
2.2
3.0
3.8
100
10
100
C
25
C
3.5 V
4.5 V
5 V
1.6
8
24
8
MTD20N03HDL
4
Motorola TMOS Power MOSFET Transistor Device Data
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 deter-
mined by how fast the FET input capacitance can be charged
by current from the generator.
The published capacitance data is difficult to use for calculat-
ing rise and fall because draingate capacitance varies
greatly with applied voltage. Accordingly, gate charge data is
used. In most cases, a satisfactory estimate of average input
current (IG(AV)) can be made from a rudimentary analysis of
the drive circuit so that
t = Q/IG(AV)
During the rise and fall time interval when switching a resis-
tive load, VGS remains virtually constant at a level known as
the plateau voltage, VSGP. Therefore, rise and fall times may
be approximated by the following:
tr = Q2 x RG/(VGG VGSP)
tf = Q2 x RG/VGSP
where
VGG = the gate drive voltage, which varies from zero to VGG
RG = the gate drive resistance
and Q2 and VGSP are read from the gate charge curve.
During the turnon and turnoff delay times, gate current is
not constant. The simplest calculation uses appropriate val-
ues from the capacitance curves in a standard equation for
voltage change in an RC network. The equations are:
td(on) = RG Ciss In [VGG/(VGG VGSP)]
td(off) = RG Ciss In (VGG/VGSP)
The capacitance (Ciss) is read from the capacitance curve at
a voltage corresponding to the offstate condition when cal-
culating td(on) and is read at a voltage corresponding to the
onstate when calculating td(off).
At high switching speeds, parasitic circuit elements com-
plicate 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 func-
tion 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 mea-
sure and, consequently, is not specified.
The resistive switching time variation versus gate resis-
tance (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 op-
erated into an inductive load; however, snubbing reduces
switching losses.
GATETOSOURCE OR DRAINTOSOURCE VOLTAGE (Volts)
C, CAP
ACIT
ANCE (pF)
Figure 7. Capacitance Variation
10
0
10
15
20
25
2800
2000
1200
400
0
VGS
VDS
1600
800
5
5
2400
VDS = 0 V
Ciss
Crss
VGS = 0 V
Ciss
Coss
Crss
TJ = 25
C
MTD20N03HDL
5
Motorola TMOS Power MOSFET Transistor Device Data
QG, TOTAL GATE CHARGE (nC)
RG, GATE RESISTANCE (Ohms)
t,
TIME (ns)
V
DS
, DRAINT
OSOURCE VOL
T
AGE (VOL
TS)
V
GS
, GA
TET
OSOURCE VOL
T
AGE (VOL
TS)
Figure 8. GateToSource and DrainToSource
Voltage versus Total Charge
1
10
100
1000
100
10
VDD = 15 V
ID = 20 A
VGS = 5.0 V
TJ = 25
C
tr
tf
td(on)
td(off)
Figure 9. Resistive Switching Time
Variation versus Gate Resistance
0
2
4
8
12
14
6
10
10
6
2
0
8
4
14
28
20
16
12
4
8
0
QT
Q2
VGS
ID = 20 A
TJ = 25
C
VDS
Q3
Q1
24
12
DRAINTOSOURCE 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 re-
covery 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 de-
vice, 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 ring-
ing. 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 con-
trolled by the device clearing the stored charge. However,
the positive di/dt during tb is an uncontrollable diode charac-
teristic 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 re-
covery 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 gen-
erated. In addition, power dissipation incurred from switching
the diode will be less due to the shorter recovery time and
lower switching losses.
I S
, SOURCE CURRENT
(AMPS)
VSD, SOURCETODRAIN VOLTAGE (Volts)
0.50
0.70
0.90
0
8
12
16
20
Figure 10. Diode Forward Voltage versus Current
4
0.60
0.80
VGS = 0 V
TJ = 25
C
1.0
0.65
0.85
0.55
0.75
0.95