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MTD1N50E

Power Field-Effect Transistor, 1A I(D), 500V, 5ohm, 1-Element, N-Channel, Silicon, Metal-oxide Semiconductor FET

器件类别:分立半导体    晶体管   

厂商名称:Motorola ( NXP )

厂商官网:https://www.nxp.com

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器件参数
参数名称
属性值
是否Rohs认证
不符合
厂商名称
Motorola ( NXP )
包装说明
SMALL OUTLINE, R-PSSO-G2
Reach Compliance Code
unknown
Is Samacsys
N
其他特性
AVALANCHE RATED
雪崩能效等级(Eas)
45 mJ
外壳连接
DRAIN
配置
SINGLE
最小漏源击穿电压
500 V
最大漏极电流 (Abs) (ID)
1 A
最大漏极电流 (ID)
1 A
最大漏源导通电阻
5 Ω
FET 技术
METAL-OXIDE SEMICONDUCTOR
JESD-30 代码
R-PSSO-G2
JESD-609代码
e0
元件数量
1
端子数量
2
工作模式
ENHANCEMENT MODE
最高工作温度
150 °C
封装主体材料
PLASTIC/EPOXY
封装形状
RECTANGULAR
封装形式
SMALL OUTLINE
极性/信道类型
N-CHANNEL
最大功率耗散 (Abs)
40 W
最大脉冲漏极电流 (IDM)
3 A
认证状态
Not Qualified
表面贴装
YES
端子面层
Tin/Lead (Sn/Pb)
端子形式
GULL WING
端子位置
SINGLE
晶体管应用
SWITCHING
晶体管元件材料
SILICON
Base Number Matches
1
文档预览
MOTOROLA
SEMICONDUCTOR TECHNICAL DATA
Order this document
by MTD1N50E/D
Data Sheet
TMOS E-FET.
Power Field Effect Transistor
DPAK for Surface Mount
Designer's
MTD1N50E
Motorola Preferred Device
N–Channel Enhancement–Mode Silicon Gate
This high voltage MOSFET uses an advanced termination
scheme to provide enhanced voltage–blocking capability without
degrading performance over time. In addition this advanced TMOS
E–FET is designed to withstand high energy in the avalanche and
commutation modes. The new energy efficient design also offers a
drain–to–source diode with a fast recovery time. Designed for high
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.
Robust High Voltage Termination
Avalanche Energy Specified
Source–to–Drain Diode Recovery Time Comparable to a
Discrete 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, 13–inch/2500
Unit Tape & Reel, Add –T4 Suffix to Part Number
G
S
TMOS POWER FET
1.0 AMPERE
500 VOLTS
RDS(on) = 5.0 OHM
®
D
CASE 369A–13, Style 2
DPAK
MAXIMUM RATINGS
(TC = 25°C unless otherwise noted)
Rating
Drain–to–Source Voltage
Drain–to–Gate Voltage (RGS = 1.0 MΩ)
Gate–to–Source Voltage — Continuous
— Non–repetitive (tp
10 ms)
Drain Current — Continuous
— Continuous @ 100°C
— Single Pulse (tp
10
µs)
Total Power Dissipation @ TC = 25°C
Derate above 25°C
Total Power Dissipation @ TA = 25°C, when mounted to minimum recommended pad size
Operating and Storage Temperature Range
Single Pulse Drain–to–Source Avalanche Energy — Starting TJ = 25°C
(VDD = 100 Vdc, VGS = 10 Vdc, IL = 3.0 Apk, L = 10 mH, RG = 25
Ω)
Thermal Resistance — Junction to Case
— Junction to Ambient
— Junction to Ambient, when mounted to minimum recommended pad size
Maximum Temperature for Soldering Purposes, 1/8″ from case for 10 seconds
Symbol
VDSS
VDGR
VGS
VGSM
ID
ID
IDM
PD
Value
500
500
±20
±40
1.0
0.8
3.0
40
0.32
1.75
– 55 to 150
45
3.13
100
71.4
260
Unit
Vdc
Vdc
Vdc
Vpk
Adc
Apk
Watts
W/°C
Watts
°C
mJ
°C/W
TJ, Tstg
EAS
R
θJC
R
θJA
R
θJA
TL
°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.
E–FET and Designer’s 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
©
Motorola TMOS
Motorola, Inc. 1995
Power MOSFET Transistor Device Data
1
MTD1N50E
ELECTRICAL CHARACTERISTICS
(TJ = 25°C unless otherwise noted)
Characteristic
OFF CHARACTERISTICS
Drain–Source Breakdown Voltage
(VGS = 0 Vdc, ID = 0.25
µAdc)
Temperature Coefficient (Positive)
Zero Gate Voltage Drain Current
(VDS = 500 Vdc, VGS = 0 Vdc)
(VDS = 500 Vdc, VGS = 0 Vdc, TJ = 125°C)
Gate–Body Leakage Current (VGS =
±
20 Vdc, VDS = 0)
ON CHARACTERISTICS (1)
Gate Threshold Voltage
(VDS = VGS, ID = 250
µAdc)
Temperature Coefficient (Negative)
Static Drain–Source On–Resistance (VGS = 10 Vdc, ID = 0.5 Adc)
Drain–Source On–Voltage (VGS = 10 Vdc)
(ID = 1.0 Adc)
(ID = 0.5 Adc, TJ = 125°C)
Forward Transconductance (VDS = Vdc, ID = 0.5 Adc)
DYNAMIC CHARACTERISTICS
Input Capacitance
Output Capacitance
Reverse Transfer Capacitance
SWITCHING CHARACTERISTICS (2)
Turn–On Delay Time
Rise Time
Turn–Off Delay Time
Fall Time
Gate Charge
(See Figure 8)
(VDS = 400 Vdc, ID = 1.0 Adc,
VGS = 10 Vdc)
(VDD = 250 Vdc, ID = 1.0 Adc,
VGS = 10 Vdc,
RG = 9.1
Ω)
td(on)
tr
td(off)
tf
QT
Q1
Q2
Q3
SOURCE–DRAIN DIODE CHARACTERISTICS
Forward On–Voltage (1)
(IS = 1.0 Adc, VGS = 0 Vdc)
(IS = 1.0 Adc, VGS = 0 Vdc, TJ = 125°C)
VSD
trr
(IS = 1.0 Adc, VGS = 0 Vdc,
dIS/dt = 100 A/µs)
Reverse Recovery Stored Charge
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.
LD
LS
3.5
4.5
7.5
nH
nH
ta
tb
QRR
0.81
0.68
141
82
58.5
0.65
1.2
µC
ns
Vdc
8.0
9.0
14
17
7.4
1.6
3.8
5.0
20
10
30
30
9.0
nC
ns
(VDS = 25 Vdc, VGS = 10 Vdc,
f = 1.0 MHz)
Ciss
Coss
Crss
215
30.2
6.7
315
42
12
pF
VGS(th)
2.0
RDS(on)
VDS(on)
gFS
0.5
4.5
0.9
6.0
5.3
mhos
3.2
6.0
4.3
4.0
5.0
Vdc
mV/°C
Ohm
Vdc
V(BR)DSS
500
IDSS
IGSS
10
100
100
nAdc
480
Vdc
mV/°C
µAdc
Symbol
Min
Typ
Max
Unit
Reverse Recovery Time
(See Figure 14)
2
Motorola TMOS Power MOSFET Transistor Device Data
MTD1N50E
TYPICAL ELECTRICAL CHARACTERISTICS
2.0
1.75
I D , DRAIN CURRENT (AMPS)
1.50
1.25
1.0
0.75
0.50
0.25
0
0
2
4
6
8
10
12
14
16
5V
TJ = 25°C
VGS = 10 V
8V
7V
6V
I D , DRAIN CURRENT (AMPS)
2.0
1.75
1.50
1.25
1.0
0.75
0.50
0.25
– 55°C
0
2.0
2.5
3.0
3.5
4.0
4.5
5.0
5.5
6.0
6.5
TJ = 100°C
25°C
VDS
10 V
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS)
VGS, GATE–TO–SOURCE VOLTAGE (VOLTS)
Figure 1. On–Region Characteristics
R DS(on) , DRAIN–TO–SOURCE RESISTANCE (OHMS)
R DS(on) , DRAIN–TO–SOURCE RESISTANCE (OHMS)
Figure 2. Transfer Characteristics
10
VGS = 10 V
8
TJ = 100°C
6.0
TJ = 25°C
5.5
5.0
VGS = 10 V
4.5
4.0
3.5
3.0
0
0.25
0.50
0.75
1.0
1.25
1.50
1.75
2.0
ID, DRAIN CURRENT (AMPS)
15 V
6
25°C
4
– 55°C
2
0
0
0.4
0.8
1.2
1.6
2.0
ID, DRAIN CURRENT (AMPS)
Figure 3. On–Resistance versus Drain Current
and Temperature
Figure 4. On–Resistance versus Drain Current
and Gate Voltage
RDS(on) , DRAIN–TO–SOURCE RESISTANCE
(NORMALIZED)
2.5
VGS = 10 V
ID = 0.5 A
10000
VGS = 0 V
1000
TJ = 125°C
2.0
1.5
I DSS , LEAKAGE (nA)
100°C
100
1.0
10
25°C
0.5
0
– 50
– 25
0
25
50
75
100
125
150
1
0
100
200
300
400
500
TJ, JUNCTION TEMPERATURE (°C)
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS)
Figure 5. On–Resistance Variation with
Temperature
Figure 6. Drain–To–Source Leakage
Current versus Voltage
Motorola TMOS Power MOSFET Transistor Device Data
3
MTD1N50E
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 drain–gate 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 turn–on and turn–off 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)
500
450
400
C, CAPACITANCE (pF)
C, CAPACITANCE (pF)
350
300
250
200
150
100
50
0
10
5
VGS
0
VDS
Crss
Crss
5
10
Coss
15
20
25
1
10
100
VDS, DRAIN–TO–SOURCE VOLTAGE (VOLTS)
1000
Ciss
Ciss
100
VDS = 0 V
VGS = 0 V
TJ = 25°C
The capacitance (Ciss) is read from the capacitance curve at
a voltage corresponding to the off–state condition when cal-
culating td(on) and is read at a voltage corresponding to the
on–state 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.
1000
VGS = 0 V
TJ = 25°C
Ciss
Coss
10
Crss
GATE–TO–SOURCE OR DRAIN–TO–SOURCE VOLTAGE (VOLTS)
Figure 7a. Capacitance Variation
Figure 7b. High Voltage Capacitance
Variation
4
Motorola TMOS Power MOSFET Transistor Device Data
MTD1N50E
VDS , DRAIN–TO–SOURCE VOLTAGE (VOLTS)
VGS, GATE–TO–SOURCE VOLTAGE (VOLTS)
12
10
8
6
4
2
0
0
2
Q3
4
QT, TOTAL CHARGE (nC)
6
Q1
Q2
QT
VGS
240
180
120
60
0
8
360
300
100
VDD = 250 V
ID = 1 A
VGS = 10 V
TJ = 25°C
t, TIME (ns)
tf
10
td(off)
td(on)
tr
ID = 1 A
TJ = 25°C
VDS
1
1
10
RG, GATE RESISTANCE (OHMS)
100
Figure 8. Gate–To–Source and Drain–To–Source
Voltage versus Total Charge
Figure 9. Resistive Switching Time
Variation versus Gate Resistance
DRAIN–TO–SOURCE DIODE CHARACTERISTICS
1.0
I S , SOURCE CURRENT (AMPS)
VGS = 0 V
TJ = 25°C
0.8
0.6
0.4
0.2
0
0.5
0.54
0.58
0.62
0.66
0.70
0.74
0.78
VSD, SOURCE–TO–DRAIN VOLTAGE (VOLTS)
0.82
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 av-
eraged over a complete switching cycle must not exceed
(TJ(MAX) – TC)/(R
θJC
).
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 (I DM ), 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.
Motorola TMOS Power MOSFET Transistor Device Data
5
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