Allicdata Part #: | FQPF9N50CYDTU-ND |
Manufacturer Part#: |
FQPF9N50CYDTU |
Price: | $ 0.00 |
Product Category: | Discrete Semiconductor Products |
Manufacturer: | ON Semiconductor |
Short Description: | MOSFET N-CH 500V 9A TO-220F |
More Detail: | N-Channel 500V 9A (Tc) 44W (Tc) Through Hole TO-22... |
DataSheet: | FQPF9N50CYDTU Datasheet/PDF |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | QFET® |
Packaging: | Tube |
Part Status: | Obsolete |
FET Type: | N-Channel |
Technology: | MOSFET (Metal Oxide) |
Drain to Source Voltage (Vdss): | 500V |
Current - Continuous Drain (Id) @ 25°C: | 9A (Tc) |
Drive Voltage (Max Rds On, Min Rds On): | 10V |
Rds On (Max) @ Id, Vgs: | 800 mOhm @ 4.5A, 10V |
Vgs(th) (Max) @ Id: | 4V @ 250µA |
Gate Charge (Qg) (Max) @ Vgs: | 35nC @ 10V |
Vgs (Max): | ±30V |
Input Capacitance (Ciss) (Max) @ Vds: | 1030pF @ 25V |
FET Feature: | -- |
Power Dissipation (Max): | 44W (Tc) |
Operating Temperature: | -55°C ~ 150°C (TJ) |
Mounting Type: | Through Hole |
Supplier Device Package: | TO-220F-3 (Y-Forming) |
Package / Case: | TO-220-3 Full Pack, Formed Leads |
Due to market price fluctuations, if you need to purchase or consult the price. You can contact us or emial to us: sales@allicdata.com
The FQPF9N50CYDTU is a depletion-mode, N-channel MOSFET (Metal Oxide Semiconductor Field Effect Transistor). This transistor is a voltage-driven semiconductor device that has three electrodes: its main current input (gate), the current output (source) and the body (drain). Compared to the more common BJT (Bipolar Junction Transistor) these transistors have higher impedance of their inputs and offers very low power dissipation.
The FQPF9N50CYDTU is suitable for use as an amplifier, switch, Linear control or any application where voltage needs to be used to control current flow. Some of the common applications of the FQPF9N50CYDTU include motor control, solar cell control, robotics, voltage regulators, audio signal processing, and analog signal conditioning. The FQPF9N50CYDTU is also used in DC-DC converters, high-speed switching applications and low-leakage power management designs.
The working principle of the FQPF9N50CYDTU is based on the principles of MOSFETs, wherein the voltage applied to its gate controls the current that passes through it. When the voltage on the gate is decreased, the current will also decrease. When the voltage on the gate is increased, the current will also increase. Therefore, the current can be easily controlled by varying the voltage applied to the gate.
To use this transistor, the gate voltage needs to be higher than the drain voltage by a certain amount increase (VGS(th)) in order to activate it. For the FQPF9N50CYDTU, it has an operational VGS(th) of 1.8V and a maximum VGS of ±20V. Additionally, the current across the source and drain is limited by a maximum allowable voltage, which is known as the drain-source breakdown voltage (VDSS) for the FQPF9N50CYDTU. If a higher VDSS is desired, then the power dissipation must be increased proportionately.
The FQPF9N50CYDTU also has a maximum power dissipation rating of 500 watts per device. This means that it can only handle a certain amount of power before it starts to overheat. Therefore, when using this device it is important to be aware of the amount of power that it can handle.
The FQPF9N50CYDTU also has a maximum switching speed, which is known as the turn-off time (tF). This is the amount of time it takes for the FQPF9N50CYDTU to turn off after being activated. Additionally, it also has a maximum drain-source capacitance (CGD) which limits the amount of capacitive load that can be connected to the device. The FQPF9N50CYDTU has a maximum drain-source capacitance of 4.6 pF.
In summary, the FQPF9N50CYDTU is a depletion-mode, N-channel metal oxide semiconductor field effect transistor. This device is used in a variety of applications such as motor control, solar cell control, robotics, voltage regulators, audio signal processing and analog signal conditioning. The FQPF9N50CYDTU is activated by applying a voltage greater than the operational VGS(th) of 1.8V. The amount of current passing through the device is then controlled by varying the gate voltage. The FQPF9N50CYDTU also has a maximum power dissipation rating of 500 watts per device and a maximum turn-off time (tF) of 13.5ns. Furthermore, it also has a maximum drain-source capacitance of 4.6pF.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
FQPF10N60CT | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 600V 9.5A TO-... |
FQPF11N40T | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 400V 6.6A TO-... |
FQPF12P20YDTU | ON Semicondu... | 0.0 $ | 1000 | MOSFET P-CH 200V 7.3A TO-... |
FQPF13N50CT | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 500V 13A TO-2... |
FQPF18N20V2YDTU | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 200V 18A TO-2... |
FQPF3N50C | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 500V 3A TO-22... |
FQPF6N40CF | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 400V 6A TO-22... |
FQPF7N65C_F105 | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 650V 7A TO-22... |
FQPF8N60CT | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 600V 7.5A TO-... |
FQPF9N50CYDTU | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 500V 9A TO-22... |
FQPF9N90C | ON Semicondu... | -- | 1000 | MOSFET N-CH 900V 8A TO-22... |
FQPF6N90CT | ON Semicondu... | -- | 1000 | MOSFET N-CH 900V 6A TO-22... |
FQPF3N90_NL | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 900V 2.1A TO-... |
FQPF6N90C | ON Semicondu... | -- | 302 | MOSFET N-CH 900V 6A TO-22... |
FQPF13N50CF | ON Semicondu... | -- | 952 | MOSFET N-CH 500V 13A TO-2... |
FQPF2N60C | ON Semicondu... | -- | 374 | MOSFET N-CH 600V 2A TO-22... |
FQPF9N25C | ON Semicondu... | -- | 614 | MOSFET N-CH 250V 8.8A TO-... |
FQPF5N60C | ON Semicondu... | -- | 411 | MOSFET N-CH 600V 4.5A TO-... |
FQPF13N06L | ON Semicondu... | -- | 68 | MOSFET N-CH 60V 10A TO-22... |
FQPF5N50CYDTU | ON Semicondu... | -- | 801 | MOSFET N-CH 500V 5A TO-22... |
FQPF4N90C | ON Semicondu... | -- | 1000 | MOSFET N-CH 900V 4A TO-22... |
FQPF11N40C | ON Semicondu... | -- | 656 | MOSFET N-CH 400V 10.5A TO... |
FQPF9P25 | ON Semicondu... | -- | 977 | MOSFET P-CH 250V 6A TO-22... |
FQPF8N80C | ON Semicondu... | -- | 987 | MOSFET N-CH 800V 8A TO-22... |
FQPF27N25 | ON Semicondu... | -- | 246 | MOSFET N-CH 250V 14A TO-2... |
FQPF65N06 | ON Semicondu... | -- | 442 | MOSFET N-CH 60V 40A TO-22... |
FQPF9N90CT | ON Semicondu... | -- | 613 | MOSFET N-CH 900V 8A TO-22... |
FQPF2N80 | ON Semicondu... | -- | 1000 | MOSFET N-CH 800V 1.5A TO-... |
FQPF11N50CF | ON Semicondu... | -- | 271 | MOSFET N-CH 500V 11A TO-2... |
FQPF32N20C | ON Semicondu... | -- | 43 | MOSFET N-CH 200V 28A TO-2... |
FQPF45N15V2 | ON Semicondu... | -- | 1000 | MOSFET N-CH 150V 45A TO-T... |
FQPF19N20C | ON Semicondu... | -- | 1000 | MOSFET N-CH 200V 19A TO-2... |
FQPF20N06 | ON Semicondu... | -- | 36 | MOSFET N-CH 60V 15A TO-22... |
FQPF18N50V2 | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 500V 18A TO-2... |
FQPF7N10L | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 100V 5.5A TO-... |
FQPF5N20L | ON Semicondu... | 0.0 $ | 1000 | MOSFET N-CH 200V 3.5A TO-... |
FQPF5N15 | ON Semicondu... | -- | 1000 | MOSFET N-CH 150V 4.2A TO-... |
FQPF7P06 | ON Semicondu... | 0.0 $ | 1000 | MOSFET P-CH 60V 5.3A TO-2... |
FQPF5N20 | ON Semicondu... | -- | 1000 | MOSFET N-CH 200V 3.5A TO-... |
FQPF4N20 | ON Semicondu... | -- | 1000 | MOSFET N-CH 200V 2.8A TO-... |
MOSFET N-CH 200V 31A D2PAKN-Channel 200V...
MOSFET N-CH 55V 440A TO-268N-Channel 55V...
MOSFET N-CH 800V 14A TO-247N-Channel 800...
MOSFET N-CH 600V 23A TO-268(D3)N-Channel...
MOSFET N-CH 200V 72A TO-268N-Channel 200...
MOSFET N-CH 800V 9A TO-268N-Channel 800V...