ETC NTP30N20

NTP30N20
Preferred Device
Advance Information
Power MOSFET
30 Amps, 200 Volts
N–Channel Enhancement–Mode TO–220
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Features
• Source–to–Drain Diode Recovery Time Comparable to a Discrete
30 AMPERES
200 VOLTS
68 mΩ @ VGS = 10 V (Typ)
Fast Recovery Diode
• Avalanche Energy Specified
• IDSS and RDS(on) Specified at Elevated Temperature
Typical Applications
• PWM Motor Controls
• Power Supplies
• Converters
N–Channel
D
MAXIMUM RATINGS (TC = 25°C unless otherwise noted)
Symbol
Value
Unit
Drain–to–Source Voltage
VDSS
200
Vdc
Drain–to–Source Voltage (RGS = 1.0 MΩ)
VDGR
200
Vdc
Gate–to–Source Voltage
– Continuous
– Non–Repetitive (tp10 ms)
VGS
VGSM
30
40
Rating
Drain Current
– Continuous @ TA 25°C
– Continuous @ TA 100°C
– Pulsed (Note 1)
Total Power Dissipation @ TA = 25°C
Derate above 25°C
MARKING DIAGRAM
& PIN ASSIGNMENT
4
Drain
Adc
ID
ID
IDM
30
22
90
4
214
1.43
W
W/°C
Operating and Storage Temperature Range
TJ, Tstg
–55 to
+175
°C
Single Drain–to–Source Avalanche Energy –
Starting TJ = 25°C
(VDD = 100 Vdc, VGS = 10 Vdc,
IL(pk) = 20 A, L = 3.0 mH, RG = 25 Ω)
EAS
Maximum Lead Temperature for Soldering
Purposes, 1/8″ from case for 10 seconds
S
Vdc
PD
Thermal Resistance
– Junction–to–Case
– Junction–to–Ambient
G
mJ
450
TO–220AB
CASE 221A
STYLE 5
1
NTP30N20
LLYWW
1
Gate
2
3
3
Source
2
Drain
°C/W
RθJC
RθJA
0.7
62.5
TL
260
°C
1. Pulse Test: Pulse Width = 10 µs, Duty Cycle = 2%.
NTP30N20
LL
Y
WW
= Device Code
= Location Code
= Year
= Work Week
ORDERING INFORMATION
Device
NTP30N20
Package
Shipping
TO–220AB
50 Units/Rail
Preferred devices are recommended choices for future use
and best overall value.
This document contains information on a new product. Specifications and information
herein are subject to change without notice.
 Semiconductor Components Industries, LLC, 2002
February, 2002 – Rev. 2
1
Publication Order Number:
NTP30N20/D
NTP30N20
ELECTRICAL CHARACTERISTICS (TC = 25°C unless otherwise noted)
Characteristic
Symbol
Min
Typ
Max
Unit
200
–
–
307
–
–
–
–
–
–
5.0
125
–
–
±100
2.0
–
2.9
–8.9
4.0
–
–
–
–
0.068
0.067
0.200
0.081
0.080
0.240
–
2.0
2.5
gFS
–
20
–
mhos
pF
OFF CHARACTERISTICS
Drain–to–Source Breakdown Voltage
(VGS = 0 Vdc, ID = 250 µAdc)
Temperature Coefficient (Positive)
V(BR)DSS
Zero Gate Voltage Collector Current
(VGS = 0 Vdc, VDS = 200 Vdc, TJ = 25°C)
(VGS = 0 Vdc, VDS = 200 Vdc, TJ = 175°C)
IDSS
Gate–Body Leakage Current (VGS = ±30 Vdc, VDS = 0)
IGSS
Vdc
mV/°C
µAdc
nAdc
ON CHARACTERISTICS
Gate Threshold Voltage
VDS = VGS, ID = 250 µAdc)
Temperature Coefficient (Negative)
VGS(th)
Static Drain–to–Source On–State Resistance
(VGS = 10 Vdc, ID = 15 Adc)
(VGS = 10 Vdc, ID = 10 Adc)
(VGS = 10 Vdc, ID = 15 Adc, TJ = 175°C)
RDS(on)
Drain–to–Source On–Voltage
(VGS = 10 Vdc, ID = 30 Adc)
VDS(on)
Forward Transconductance (VDS = 15 Vdc, ID = 15 Adc)
Vdc
mV/°C
Ω
Vdc
DYNAMIC CHARACTERISTICS
Input Capacitance
(VDS = 25 Vdc, VGS = 0 Vdc, f = 1.0 MHz)
Ciss
–
2335
–
Output Capacitance
(VDS = 25 Vdc, VGS = 0 Vdc, f = 1.0 MHz)
(VDS = 160 Vdc, VGS = 0 Vdc, f = 1.0 MHz)
Coss
–
–
380
148
–
–
Reverse Transfer Capacitance
(VDS = 25 Vdc, VGS = 0 Vdc, f = 1.0 MHz)
Crss
–
75
–
td(on)
–
–
10
12
–
–
SWITCHING CHARACTERISTICS (Notes 2 & 3)
Turn–On Delay Time
ns
Rise Time
(VDD = 100 Vdc, ID = 18 Adc,
VGS = 5.0 Vdc,, RG = 2.5 Ω))
tr
–
–
20
70
–
–
Turn–Off Delay Time
(VDD = 160 Vdc, ID = 30 Adc,
VGS = 10 Vdc, RG = 9.1 Ω)
td(off)
–
–
40
82
–
–
tf
–
–
24
88
–
–
Qtot
–
–
75
48
100
–
Qgs
–
–
20
16
–
–
Qgd
–
32
–
VSD
–
–
0.91
0.80
1.1
–
Vdc
trr
–
230
–
ns
ta
–
140
–
tb
–
85
–
QRR
–
1.85
–
Fall Time
Gate Charge
(VDS = 160 Vdc, ID = 30 Adc,
VGS = 10 Vdc)
(VDS = 160 Vdc, ID = 18 Adc,
VGS = 5.0
5 0 Vdc)
nC
BODY–DRAIN DIODE RATINGS (Note 2)
Forward On–Voltage
(IS = 30 Adc, VGS = 0 Vdc)
(IS = 30 Adc, VGS = 0 Vdc, TJ = 150°C)
Reverse Recovery Time
(IS = 30 Adc,
Ad VGS = 0 Vdc,
Vd
dIS/dt = 100 A/µs)
Reverse Recovery Stored Charge
2. Indicates Pulse Test: P. W. = 300 µs max, Duty Cycle = 2%.
3. Switching characteristics are independent of operating junction temperature.
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2
µC
NTP30N20
60
VGS = 10 V
6V
ID, DRAIN CURRENT (AMPS)
ID, DRAIN CURRENT (AMPS)
60
9V
50
TJ = 25°C
8V
40
7V
30
5V
20
10
VDS ≥ 10 V
50
40
30
20
TJ = 25°C
10
TJ = 100°C
4V
0
0
2
4
6
8
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS)
0
10
0
RDS(on), DRAIN–TO–SOURCE RESISTANCE ()
0.2
VGS = 10 V
TJ = 100°C
0.15
0.1
TJ = 25°C
0.05
0
TJ = –55°C
5
15
25
35
45
ID, DRAIN CURRENT (AMPS)
10
55
0.1
TJ = 25°C
0.09
VGS = 10 V
0.08
VGS = 15 V
0.07
0.06
0.05
5
Figure 3. On–Resistance versus Drain Current
and Temperature
15
25
35
45
ID, DRAIN CURRENT (AMPS)
55
Figure 4. On–Resistance versus Drain Current
and Gate Voltage
3
2.5
2
4
6
8
VGS, GATE–TO–SOURCE VOLTAGE (VOLTS)
Figure 2. Transfer Characteristics
100000
VGS = 0 V
ID = 15 A
VGS = 10 V
TJ = 175°C
10000
IDSS, LEAKAGE (nA)
RDS(on), DRAIN–TO–SOURCE RESISTANCE (NORMALIZED)
RDS(on), DRAIN–TO–SOURCE RESISTANCE ()
Figure 1. On–Region Characteristics
TJ = –55°C
2
1.5
1
1000
TJ = 100°C
100
0.5
0
–50 –25
0
25
50
75 100 125 150
TJ, JUNCTION TEMPERATURE (°C)
10
175
20
Figure 5. On–Resistance Variation with
Temperature
40
60
80 100 120 140 160 180 200
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS)
Figure 6. Drain–to–Source Leakage Current
versus Voltage
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3
NTP30N20
POWER MOSFET SWITCHING
The capacitance (Ciss) is read from the capacitance curve at
Switching behavior is most easily modeled and predicted
by recognizing that the power MOSFET is charge
a voltage corresponding to the off–state condition when
controlled. The lengths of various switching intervals (∆t)
calculating td(on) and is read at a voltage corresponding to the
are determined by how fast the FET input capacitance can
on–state when calculating td(off).
be charged by current from the generator.
At high switching speeds, parasitic circuit elements
complicate
the analysis. The inductance of the MOSFET
The published capacitance data is difficult to use for
source
lead,
inside the package and in the circuit wiring
calculating rise and fall because drain–gate capacitance
which
is
common
to both the drain and gate current paths,
varies greatly with applied voltage. Accordingly, gate
produces
a
voltage
at the source which reduces the gate drive
charge data is used. In most cases, a satisfactory estimate of
current.
The
voltage
is determined by Ldi/dt, but since di/dt
average input current (IG(AV)) can be made from a
is
a
function
of
drain
current, the mathematical solution is
rudimentary analysis of the drive circuit so that
complex. The MOSFET output capacitance also
t = Q/IG(AV)
complicates the mathematics. And finally, MOSFETs have
finite internal gate resistance which effectively adds to the
During the rise and fall time interval when switching a
resistance of the driving source, but the internal resistance
resistive load, VGS remains virtually constant at a level
is difficult to measure and, consequently, is not specified.
known as the plateau voltage, VSGP. Therefore, rise and fall
The resistive switching time variation versus gate
times may be approximated by the following:
resistance
(Figure 9) shows how typical switching
tr = Q2 x RG/(VGG – VGSP)
performance is affected by the parasitic circuit elements. If
tf = Q2 x RG/VGSP
the parasitics were not present, the slope of the curves would
maintain a value of unity regardless of the switching speed.
where
The circuit used to obtain the data is constructed to minimize
VGG = the gate drive voltage, which varies from zero to VGG
common inductance in the drain and gate circuit loops and
RG = the gate drive resistance
is believed readily achievable with board mounted
and Q2 and VGSP are read from the gate charge curve.
components. Most power electronic loads are inductive; the
data in the figure is taken with a resistive load, which
During the turn–on and turn–off delay times, gate current is
approximates an optimally snubbed inductive load. Power
not constant. The simplest calculation uses appropriate
MOSFETs may be safely operated into an inductive load;
values from the capacitance curves in a standard equation for
however, snubbing reduces switching losses.
voltage change in an RC network. The equations are:
td(on) = RG Ciss In [VGG/(VGG – VGSP)]
td(off) = RG Ciss In (VGG/VGSP)
6000
VDS = 0 V
C, CAPACITANCE (pF)
5000
VGS = 0 V
TJ = 25°C
Ciss
4000
3000
Crss
Ciss
2000
1000
Coss
Crss
0
0
0
5
VGS
5
10
15
20
25
VDS
GATE–TO–SOURCE OR DRAIN–TO–SOURCE VOLTAGE
(VOLTS)
Figure 7. Capacitance Variation
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4
180
QT
VDS
10
150
120
8
Q1
6
VGS
Q2
90
60
4
ID = 30 A
TJ = 25°C
2
0
0
10
20
30
40
50
QG, TOTAL GATE CHARGE (nC)
60
30
0
70
1000
VDD = 160 V
ID = 30 A
VGS = 10 V
tf
100
t, TIME (ns)
12
VDS,DRAIN–TO–SOURCE VOLTAGE (VOLTS)
VGS, GATE–TO–SOURCE VOLTAGE (VOLTS)
NTP30N20
tr
td(off)
10
1
td(on)
1
Figure 8. Gate–To–Source and Drain–To–Source
Voltage versus Total Charge
10
RG, GATE RESISTANCE (Ω)
100
Figure 9. Resistive Switching Time
Variation versus Gate Resistance
DRAIN–TO–SOURCE DIODE CHARACTERISTICS
IS, SOURCE CURRENT (AMPS)
30
VGS = 0 V
TJ = 25°C
25
20
15
10
5
0
0.5
0.6
0.7
0.8
0.9
VSD, SOURCE–TO–DRAIN VOLTAGE (VOLTS)
1
Figure 10. Diode Forward Voltage versus Current
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 (VDSS) is exceeded and the
transition time (tr,tf) do not exceed 10 µs. In addition the total
power averaged over a complete switching cycle must not
exceed (TJ(MAX) – TC)/(RθJC).
A Power MOSFET designated E–FET can be safely used
in switching circuits with unclamped inductive loads. For
reliable operation, the stored energy from circuit inductance
dissipated in the transistor while in avalanche must be less
than the rated limit and 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 12). Maximum energy at
currents below rated continuous ID can safely be assumed to
equal the values indicated.
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5
NTP30N20
I D, DRAIN CURRENT (AMPS)
1000
VGS = 20 V
SINGLE PULSE
TC = 25°C
100
10 µs
100 µs
10
1 ms
10 ms
1
RDS(on) LIMIT
THERMAL LIMIT
PACKAGE LIMIT
r(t), EFFECTIVE TRANSIENT THERMAL RESISTANCE
(NORMALIZED)
0.1
0.1
dc
1.0
10
100
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS)
1000
EAS, SINGLE PULSE DRAIN–TO–SOURCE
AVALANCHE ENERGY (mJ)
SAFE OPERATING AREA
500
ID = 30 A
400
300
200
100
0
25
Figure 11. Maximum Rated Forward Biased
Safe Operating Area
175
50
75
100
125
150
TJ, STARTING JUNCTION TEMPERATURE (°C)
Figure 12. Maximum Avalanche Energy versus
Starting Junction Temperature
1.0
D = 0.5
0.2
0.1
0.1
P(pk)
0.05
0.02
t1
0.01
t2
DUTY CYCLE, D = t1/t2
SINGLE PULSE
0.01
0.00001
0.0001
0.001
0.01
t, TIME (µs)
RθJC(t) = r(t) RθJC
D CURVES APPLY FOR POWER
PULSE TRAIN SHOWN
READ TIME AT t1
TJ(pk) – TC = P(pk) RθJC(t)
0.1
Figure 13. Thermal Response
di/dt
IS
trr
ta
tb
TIME
0.25 IS
tp
IS
Figure 14. Diode Reverse Recovery Waveform
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6
1.0
10
NTP30N20
PACKAGE DIMENSIONS
TO–220 THREE–LEAD
TO–220AB
CASE 221A–09
ISSUE AA
SEATING
PLANE
–T–
B
C
F
T
S
4
DIM
A
B
C
D
F
G
H
J
K
L
N
Q
R
S
T
U
V
Z
A
Q
1 2 3
U
H
K
Z
L
R
V
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.
J
G
D
N
INCHES
MIN
MAX
0.570
0.620
0.380
0.405
0.160
0.190
0.025
0.035
0.142
0.147
0.095
0.105
0.110
0.155
0.018
0.025
0.500
0.562
0.045
0.060
0.190
0.210
0.100
0.120
0.080
0.110
0.045
0.055
0.235
0.255
0.000
0.050
0.045
----0.080
STYLE 5:
PIN 1.
2.
3.
4.
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7
GATE
DRAIN
SOURCE
DRAIN
MILLIMETERS
MIN
MAX
14.48
15.75
9.66
10.28
4.07
4.82
0.64
0.88
3.61
3.73
2.42
2.66
2.80
3.93
0.46
0.64
12.70
14.27
1.15
1.52
4.83
5.33
2.54
3.04
2.04
2.79
1.15
1.39
5.97
6.47
0.00
1.27
1.15
----2.04
NTP30N20
ON Semiconductor and
are trademarks of Semiconductor Components Industries, LLC (SCILLC). SCILLC reserves the right to make changes
without further notice to any products herein. SCILLC makes no warranty, representation or guarantee regarding the suitability of its products for any particular
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including without limitation special, consequential or incidental damages. “Typical” parameters which may be provided in SCILLC 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
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8
NTP30N20/D