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AP70N10F Datasheet(PDF) 2 Page - A POWER MICROELECTRONICS

Part # AP70N10F
Description  100V N-Channel Enhancement Mode MOSFET
PDF  7 Pages
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Manufacturer  APME [A POWER MICROELECTRONICS]
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AP70N10F Datasheet(HTML) 2 Page - A POWER MICROELECTRONICS

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AP70N10FIPIT
100V N-Channel Enhancement Mode MOSFET
AP70N10F/P/T RVE1.1
永源微電子科技有限公司
Electrical Characteristics@Tj=25oC(unless otherwise specified)
Symbol
Parameter
Conditions
Min.
Typ.
Max.
Unit
BVDSS
Drain-Source Breakdown Voltage
VGS=0V , ID=250uA
100
110
---
V
RDS(ON)
Static Drain-Source On-Resistance2
VGS=10V , ID=30A
---
18
25
mΩ
VGS(th)
Gate Threshold Voltage
VGS=VDS , ID =250uA
2.0
3.0
4.0
V
IDSS
Drain-Source Leakage Current
VDS=80V , VGS=0V , TJ=25
℃
---
---
1
uA
VDS=80V , VGS=0V , TJ=55
℃
---
---
5
IGSS
Gate-Source Leakage Current
VGS=±20V , VDS=0V
---
---
±100
nA
gfs
Forward Transconductance
VDS=5V , ID=30A
---
31
---
S
Rg
Gate Resistance
VDS=0V , VGS=0V , f=1MHz
---
1.9
3.8
Ω
Qg
Total Gate Charge (10V)
VDS=80V , VGS=10V , ID=30A
---
27.6
---
nC
Qgs
Gate-Source Charge
---
11.4
---
Qgd
Gate-Drain Charge
---
7.9
---
Td(on)
Turn-On Delay Time
VDD=50V , VGS=10V
, RG=3.3Ω,
ID=30A
---
16.5
---
ns
Tr
Rise Time
---
35
---
Td(off)
Turn-Off Delay Time
---
17.5
---
Tf
Fall Time
---
12
---
Ciss
Input Capacitance
VDS=15V , VGS=0V , f=1MHz
---
1890
---
pF
Coss
Output Capacitance
---
268
---
Crss
Reverse Transfer Capacitance
---
67
---
IS
Continuous Source Current1,5
VG=VD=0V , Force Current
---
---
58
A
ISM
Pulsed Source Current2,5
---
---
130
A
VSD
Diode Forward Voltage2
VGS=0V , IS=1A , TJ=25
℃
---
---
1.2
V
trr
Reverse Recovery Time
IF=30A , dI/dt=100A/µs ,
TJ=25
℃
---
22
---
nS
Qrr
Reverse Recovery Charge
---
20
---
nC
Note :
1、The data tested by surface mounted on a 1 inch 2 FR-4 board with 2OZ copper.
2、The data tested by pulsed , pulse width
≦ 300us , duty cycle ≦ 2%
3、The EAS data shows Max. rating . The test condition is VDD=72V,VGS=10V,L=0.1mH,IAS=40A
4、The power dissipation is limited by 150
℃ junction temperature
5、The data is theoretically the same as I D and I DM , in real applications , should be limited by total power dissipation.



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