SiC Power Series, FET, MOSFET Arrays

Results:
5
Manufacturer
Series
Current - Continuous Drain (Id) @ 25°C
Input Capacitance (Ciss) (Max) @ Vds
Gate Charge (Qg) (Max) @ Vgs
Rds On (Max) @ Id, Vgs
Power - Max
FET Type
Vgs(th) (Max) @ Id
Drain to Source Voltage (Vdss)
Operating Temperature
FET Feature
Mounting Type
Supplier Device Package
Package / Case
Results remaining5
Applied Filters:
SiC Power
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ImageProduct DetailPriceAvailabilityECAD ModelMounting TypePackage / CaseSupplier Device PackageSeriesFET TypeFET FeatureDrain to Source Voltage (Vdss)Current - Continuous Drain (Id) @ 25°CRds On (Max) @ Id, VgsVgs(th) (Max) @ IdGate Charge (Qg) (Max) @ VgsInput Capacitance (Ciss) (Max) @ VdsPower - MaxOperating Temperature
GE12047CCA3
1200V 475A SIC HALF-BRIDGE
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Quantity
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PCB Symbol, Footprint & 3D Model
Chassis Mount
Module
-
SiC Power
2 N-Channel (Half Bridge)
Silicon Carbide (SiC)
1200V (1.2kV)
475A
4.4mOhm @ 475A, 20V
4.5V @ 160mA
1248nC @ 18V
29300pF @ 600V
1250W
-55°C ~ 150°C (Tc)
GE12160CEA3
1200V 1425A SiC Half-Bridge
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Quantity
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PCB Symbol, Footprint & 3D Model
Chassis Mount
Module
-
SiC Power
2 N-Channel (Half Bridge)
Silicon Carbide (SiC)
1200V (1.2kV)
1.425kA (Tc)
1.5mOhm @ 475A, 20V
4.5V @ 480mA
3744nC @ 18V
90000pF @ 600V
3.75kW (Tc)
-55°C ~ 150°C (Tc)
GE17080CDA3
1700V 765A SIC HALF-BRIDGE MODUL
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Quantity
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PCB Symbol, Footprint & 3D Model
Chassis Mount
Module
-
SiC Power
2 N-Channel (Half Bridge)
Silicon Carbide (SiC)
1200V (1.2kV)
765A
2.23mOhm @ 765A, 20V
4.5V @ 160mA
2414nC @ 18V
58000pF @ 900V
2350W
-55°C ~ 150°C (Tc)
GE12050EEA3
1200V 475A 6-Pack SiC Module
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Quantity
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PCB Symbol, Footprint & 3D Model
Chassis Mount
Module
-
SiC Power
6 N-Channel (3-Phase Bridge)
Silicon Carbide (SiC)
1200V (1.2kV)
475A (Tc)
4.4mOhm @ 475A, 20V
4.5V @ 160mA
1248nC @ 18V
29300pF @ 600V
1250W (Tc)
-55°C ~ 150°C (Tc)
GE17045EEA3
1700V 425A SiC Six-Pack Module
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Quantity
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PCB Symbol, Footprint & 3D Model
Chassis Mount
Module
-
SiC Power
6 N-Channel (3-Phase Bridge)
Silicon Carbide (SiC)
1700V (1.7kV)
425A (Tc)
4.45mOhm @ 425A, 20V
4.5V @ 160mA
1207nC @ 18V
29100pF @ 900V
1250W (Tc)
-55°C ~ 150°C (Tc)

FET, MOSFET Arrays

Field-effect transistors (FETs) are electronic devices that utilize an electric field to regulate the flow of current. By applying a voltage to the gate terminal, the conductivity between the drain and source terminals can be modified. Unlike bipolar junction transistors, FETs are unipolar transistors, which means they rely on a single type of charge carrier for their operation. This can either be electrons or holes, but not both. One of the key advantages of FETs is their high input impedance at low frequencies. This property arises due to the fact that the gate terminal of an FET doesn't draw any current, as it's designed to function in a voltage-driven mode. As a result, the input impedance of an FET can be several orders of magnitude greater than that of a similarly configured bipolar transistor. Field-effect transistors come in various types, with the most common ones being Junction FETs (JFETs) and Metal Oxide Semiconductor FETs (MOSFETs). JFETs employ a reverse-biased pn-junction to control the flow of current, while MOSFETs use an oxide layer to insulate the gate from the channel region. FETs have numerous applications in electronics, including amplifiers, switches, oscillators, and voltage regulators. Due to their high input impedance, FETs are often used in circuits where low power consumption and minimal loading effects are crucial considerations. In summary, field-effect transistors (FETs) are electronic devices that utilize an electric field to control current flow. They are unipolar transistors that rely on a single type of charge carrier for their operation. FETs offer high input impedance at low frequencies, making them ideal for use in low power applications where signal quality is a critical factor.