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SSM3055L Datasheet(PDF) 2 Page - SeCoS Halbleitertechnologie GmbH

Part # SSM3055L
Description  N-Channel Enhancement Mode MOSFET
PDF  4 Pages
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Manufacturer  SECOS [SeCoS Halbleitertechnologie GmbH]
Direct Link  http://www.secosgmbh.com
Logo SECOS - SeCoS Halbleitertechnologie GmbH

SSM3055L Datasheet(HTML) 2 Page - SeCoS Halbleitertechnologie GmbH

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Any changes of specification will not be informed individually.
Elektronische Bauelemente
SSM3055L
2.8A , 60V , RDS(ON) 100 mΩ
Ω
Ω
Ω
N-Channel Enhancement Mode MOSFET
26-Jul-2013 Rev. A
Page 2 of 4
ELECTRICAL CHARACTERISTICS (TA=25°C unless otherwise specified)
Parameter
Symbol
Min.
Typ.
Max.
Unit
Teat Conditions
Static
Drain-Source Breakdown Voltage
BVDSS
60
-
-
V
VGS=0, ID=250µA
Gate-Threshold Voltage
VGS(th)
1
-
2.5
V
VDS=VGS, ID=250µA
Gate-Body Leakage Current
IGSS
-
-
±100
nA
VGS=±20V
TJ=25°C
-
-
1
V DS=48V, VGS=0
Drain-Source Leakage
Current
TJ=55°C
IDSS
-
-
5
µA
VDS=48V, VGS=0
-
-
100
VGS=10V, ID=2.5A
Drain-Source On-Resistance
2
RDS(ON)
-
-
110
m
VGS=4.5V, ID=2A
Total Gate Charge
Qg
-
5
-
Gate-Source Charge
Qgs
-
1.68
-
Gate-Drain (‘’Miller’’)Charge
Qgd
-
1.9
-
nC
VDS=48V,
VGS=4.5V,
ID=2A
Turn-on Delay Time
2
Td(on)
-
1.6
-
Rise Time
Tr
-
7.2
-
Turn-off Delay Time
Td(off)
-
25
-
Fall Time
Tf
-
14.4
-
nS
VDD=30V,
VGS=10V,
RG=3.3 ,
ID=2A
Input Capacitance
Ciss
-
511
-
Output Capacitance
Coss
-
38
-
Reverse Transfer Capacitance
Crss
-
25
-
pF
VGS=0,
VDS=15V,
f=1.0MHz
Source-Drain Diode
Diode Forward Voltage
2
VSD
-
-
1.2
V
IS=1A, VGS=0
Continuous Source Current
1.4
IS
-
-
2.8
Pulsed Source Current
2.4
ISM
-
-
12
A
VG=VD=0, Force Current
Reverse Recovery Time
TRR
-
9.7
-
nS
Reverse Recovery Charge
QRR
-
5.8
-
nC
IS=2A, dI/dt=100A/µs
VGS=0
Notes:
1.
Surface mounted on a 1 inch2 FR4 board with 2OZ copper, t≦10sec., 125°C /W when mounted on Min. copper pad.
2.
The data tested by pulsed , pulse width≦300µs, duty cycle≦2%
3.
The power dissipation is limited by 150 °C junc tion temperature
4.
The data is theoretically the same as ID and IDM , in real applications , should be limited by total power dissipation



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