ON Semiconductor NTP27N06, NTB27N06 Technical data

查询NTB27N06供应商
NTP27N06, NTB27N06
Power MOSFET 27 Amps, 60 Volts
N–Channel TO–220 and D2PAK
Designed for low voltage, high speed switching applications in
power supplies, converters, power motor controls and bridge circuits.
Features
Higher Current Rating
Lower R
Lower V
Lower Capacitances
T ypical Applications
Power Supplies
Converters
Power Motor Controls
Bridge Circuits
MAXIMUM RATINGS (T
Drain–to–Source Voltage V Drain–to–Gate Voltage (RGS = 10 MΩ) V Gate–to–Source Voltage
Drain Current
Total Power Dissipation @ TA = 25°C
Operating and Storage Temperature Range TJ, T
Single Pulse Drain–to–Source Avalanche
Thermal Resistance – Junction–to–Case R Maximum Lead Temperature for Soldering
DS(on) DS(on)
= 25°C unless otherwise noted)
C
Rating Symbol Value Unit
– Continuous – Non–Repetitive (tp10 ms)
– Continuous @ TA = 25°C – Continuous @ TA 100°C – Single Pulse (tp10 µs)
Derate above 25°C
Energy – Starting TJ = 25°C (VDD = 50 Vdc, VGS = 10 Vdc, L = 0.3 mH, IL(pk) = 27 A,VDS = 60 Vdc)
Purposes, 1/8 from case for 10 seconds
DSS
DGR
V
GS
V
GS
I
D
I
D
I
DM P
E
AS
θJC
T
60 Vdc 60 Vdc
2030
27 15 80
stg
88.2
0.59WW/°C
–55 to
+175
109 mJ
1.7 °C/W
260 °C
D
L
Vdc
Adc
Apk
°C
1
Gate
2
1
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27 AMPERES
60 VOLTS
R
DS(on)
N–Channel
G
4
TO–220AB
CASE 221A
STYLE 5
3
MARKING DIAGRAMS
& PIN ASSIGNMENTS
4
Drain
NTx27N06 LLYWW
3 Source
2
Drain
= 46 m
D
S
1
2
3
D2PAK
CASE 418B
STYLE 2
4
Drain
NTx27N06 LLYWW
2
1
Drain
Gate
NTx27N06 = Device Code x = B or P LL = Location Code Y = Year WW = Work Week
4
3 Source
Semiconductor Components Industries, LLC, 2001
August, 2001 – Rev. 2
ORDERING INFORMATION
Device Package Shipping
NTP27N06 TO–220AB 50 Units/Rail NTB27N06 D2PAK 50 Units/Rail NTB27N06T4 D2PAK 800/Tape & Reel
1 Publication Order Number:
NTP27N06/D
NTP27N06, NTB27N06
)
f
MHz)
R
G
9.1 ) (Note 1.) )
V
GS
Vdc) (Note 1.)
)
dIS/dt
100 A/µs) (Note 1.)
ELECTRICAL CHARACTERISTICS (T
Characteristic
OFF CHARACTERISTICS
Drain–to–Source Breakdown Voltage (Note 1.)
(VGS = 0 Vdc, ID = 250 µAdc)
Temperature Coefficient (Positive) Zero Gate Voltage Drain Current
(VDS = 60 Vdc, VGS = 0 Vdc) (VDS = 60 Vdc, VGS = 0 Vdc, TJ = 150°C)
Gate–Body Leakage Current (VGS = ±20 Vdc, VDS = 0 Vdc) I
ON CHARACTERISTICS (Note 1.)
Gate Threshold Voltage (Note 1.)
(VDS = VGS, ID = 250 µAdc)
Threshold Temperature Coefficient (Negative) Static Drain–to–Source On–Resistance (Note 1.)
(VGS = 10 Vdc, ID = 13.5 Adc)
Static Drain–to–Source On–Resistance (Note 1.)
(VGS = 10 Vdc, ID = 27 Adc) (VGS = 10 Vdc, ID = 13.5 Adc, TJ = 150°C)
Forward Transconductance (Note 1.) (VDS = 7.0 Vdc, ID = 6.0 Adc) g
DYNAMIC CHARACTERISTICS
Input Capacitance Output Capacitance
Transfer Capacitance
SWITCHING CHARACTERISTICS (Note 2.)
Turn–On Delay Time Rise Time Turn–Off Delay Time Fall Time Gate Charge
SOURCE–DRAIN DIODE CHARACTERISTICS
Forward On–Voltage
(IS = 27 Adc, VGS = 0 Vdc, TJ = 150°C)
Reverse Recovery Time
Reverse Recovery Stored Charge Q
1. Pulse Test: Pulse Width ≤300 µs, Duty Cycle ≤ 2%.
2. Switching characteristics are independent of operating junction temperature.
= 25°C unless otherwise noted)
J
(VDS = 25 Vdc, VGS = 0 Vdc,
(IS = 27 Adc, VGS = 0 Vdc) (Note 1.)
f = 1.0 MHz
= 1.0
(VDD = 30 Vdc, ID = 27 Adc,
VGS = 10 Vdc,
RG = 9.1 ) (Note 1.)
(VDS = 48 Vdc, ID = 27 Adc,
V
= 10 Vdc) (Note 1.
= 10
(IS = 27 Adc, VGS = 0 Vdc, dI
/dt = 100 A/µs) (Note 1.
=
Symbol Min Typ Max Unit
V
(BR)DSS
I
DSS
GSS
V
GS(th)
R
DS(on)
V
DS(on)
FS
C
iss
C
oss
C
rss
t
d(on)
t
r
t
d(off)
t
f
Q
T
Q
1
Q
2
V
SD
t
rr
t
a
t
b
RR
60
– –
±100 nAdc
2.0 –
37.5 46
– –
13.2 mhos
725 1015 pF – 213 300 – 58 120
13.6 30 ns – 62.7 125 – 26.6 60 – 70.4 140 – 21.2 30 nC – 5.6 – – 7.3
– –
42 – – 26 – – 16 – – 0.07 µc
70
79.4
– –
2.8
6.9
1.05
2.12
1.05
0.93
– –
1.0 10
4.0
1.5
1.25 –
mV/°C
mV/°C
Vdc
µAdc
Vdc
m
Vdc
Vdc
ns
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2
NTP27N06, NTB27N06
56 48
40
32
24
16
, DRAIN CURRENT (AMPS)
D
8
I
0
0
VGS = 10 V
9 V
8 V
21
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS)
7.5 V
3
45
7 V
6.5 V
6 V
5.5 V
5 V
4.5 V
6
56
VDS 10 V
48
40
32
24
16
, DRAIN CURRENT (AMPS)
D
8
I
0
2.6 3.4 8.2
Figure 1. On–Region Characteristics Figure 2. Transfer Characteristics
0.095 VGS = 10 V
0.085
0.075
0.065
0.055
0.045
0.035
0.025
, DRAIN–TO–SOURCE RESISTANCE ()
0.015
032241684056
DS(on)
R
TJ = 100°C
TJ = 25°C
TJ = –55°C
48
ID, DRAIN CURRENT (AMPS)
0.095
0.085
0.075
0.065
0.055
0.045
0.035
0.025
, DRAIN–TO–SOURCE RESISTANCE ()
0.015
DS(on)
R
VGS = 15 V
032241684056
TJ = 25°C
TJ = 100°C
TJ = –55°C
4.2 5 5.8 6.6 7.4
VGS, GATE–TO–SOURCE VOLTAGE (VOLTS)
TJ = 100°C
TJ = 25°C
TJ = –55°C
48
ID, DRAIN CURRENT (AMPS)
Figure 3. On–Resistance versus
Gate–to–Source Voltage
2.2 ID = 13.5 A
VGS = 10 V
1.8
1.4
1
0.6
–50 50250–25 75 100
, DRAIN–TO–SOURCE RESISTANCE (NORMALIZED)
DS(on)
R
TJ, JUNCTION TEMPERATURE (°C)
Figure 5. On–Resistance Variation with
Temperature
10000
1000
100
, LEAKAGE (nA)
10
DSS
I
1
175150125
04050302010 60
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3
Figure 4. On–Resistance versus Drain Current
and Gate Voltage
VGS = 0 V
TJ = 150°C
TJ = 125°C
TJ = 100°C
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS)
Figure 6. Drain–to–Source Leakage Current
versus V oltage
NTP27N06, NTB27N06
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 rudimentary analysis of 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 times may 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 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
) can be made from a
G(AV)
. Therefore, rise and fall
SGP
)
)]
GSP
)
GSP
GG
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.
1800 1600
C
1400 1200 1000
C, CAPACITANCE (pF)
GATE–TO–SOURCE OR DRAIN–TO–SOURCE VOLTAGE (VOLTS)
iss
C
rss
800 600 400 200
0
10 0 10 15 20 25
55
VGS = 0 VVDS = 0 V
C
rss
V
GSVDS
Figure 7. Capacitance Variation
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4
TJ = 25°C
C
iss
C
oss
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