Allicdata Part #: | SQP10250E_GE3-ND |
Manufacturer Part#: |
SQP10250E_GE3 |
Price: | $ 2.34 |
Product Category: | Discrete Semiconductor Products |
Manufacturer: | Vishay Siliconix |
Short Description: | MOSFET N-CH 250V TO-220AB |
More Detail: | N-Channel 250V 53A (Tc) 250W (Tc) Through Hole TO-... |
DataSheet: | SQP10250E_GE3 Datasheet/PDF |
Quantity: | 1000 |
1 +: | $ 2.12310 |
10 +: | $ 1.91709 |
100 +: | $ 1.54048 |
500 +: | $ 1.19815 |
1000 +: | $ 0.99275 |
Gate Charge (Qg) (Max) @ Vgs: | 75nC @ 10V |
Package / Case: | TO-220-3 |
Supplier Device Package: | TO-220AB |
Mounting Type: | Through Hole |
Operating Temperature: | -55°C ~ 175°C (TJ) |
Power Dissipation (Max): | 250W (Tc) |
FET Feature: | -- |
Input Capacitance (Ciss) (Max) @ Vds: | 4050pF @ 25V |
Vgs (Max): | ±20V |
Series: | Automotive, AEC-Q101, TrenchFET® |
Vgs(th) (Max) @ Id: | 3.5V @ 250µA |
Rds On (Max) @ Id, Vgs: | 30 mOhm @ 15A, 10V |
Drive Voltage (Max Rds On, Min Rds On): | 7.5V, 10V |
Current - Continuous Drain (Id) @ 25°C: | 53A (Tc) |
Drain to Source Voltage (Vdss): | 250V |
Technology: | MOSFET (Metal Oxide) |
FET Type: | N-Channel |
Part Status: | Active |
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The SQP10250E_GE3 is a single N-Channel enhancement-mode, Field Effect Transistor (FET) ideal for many high-power applications. Built with a wide range of features, the SQP10250E_GE3 is widely used in power management, high-speed switching, automotive, and other industrial and consumer sectors. This article will discuss the application fields and working principles behind this highly versatile transistor.
The Application Fields and Benefits of the SQP10250E_GE3
The SQP10250E_GE3 is an N-Channel enhancement-mode, field effect transistor. This FET is built with an optimized architecture to provide superior performance in many types of applications. Some of these application fields include power management, high speed switching, automotive, and other industrial and consumer sectors.
The SQP10250E_GE3 is well suited for use in power management applications due to its robust design. With a maximum VDS of 250 volts, the device is capable of handling high electrical loads, making it an ideal choice for power management applications that require high voltage and current. Furthermore, the device has a low gate threshold voltage of 0.5 V, enabling it to be used in multiplexers and switching circuits. Additionally, the device has an RDS(on) of 12mΩ, making it suitable for low-power applications.
The SQP10250E_GE3 is also highly suitable for use in high-speed switching applications. Due to its low on-resistance values and low gate-drive, the device can be used to switch signals at high frequencies, making it an ideal choice for embedded systems, wireless communications, and motor control systems. Furthermore, the device has a low Turn-on voltage, allowing for fast and efficient switching.
The SQP10250E_GE3 has a wide range of features, making it suitable for use in a variety of automotive applications. Due to its robust design, the device is capable of withstanding high temperatures and shock, making it ideal for use in automotive systems that require high levels of reliability. Additionally, the device is RoHS compliant and features an integrated ESD protection, further adding to its versatility in automotive applications.
The SQP10250E_GE3 is also suitable for use in a variety of industrial and consumer applications. Its low on-resistance and wide operating temperature range make it well suited for use in a variety of non-automotive applications. Additionally, the device is available in a surface mount package, which makes it suitable for use in small, space-constrained applications.
The Working Principle of the SQP10250E_GE3
As an N-Channel enhancement-mode, field effect transistor, the SQP10250E_GE3 operates by manipulating electric fields. When a voltage is applied to the gate of the device, an electric field is created between the gate and the source. This field then attracts electrons from the N-Channel, creating a conducting channel between the drain and the source.
The current flowing through this channel is then regulated by the amount of voltage applied to the gate. If the gate voltage is increased, more electrons are attracted to the channel, reducing its resistance and allowing more current to flow. Similarly, if the gate voltage is decreased, electrons are repelled from the channel, increasing its resistance and reducing the amount of current flowing through the device.
The SQP10250E_GE3 also features a built-in protection mechanism in the form of the P-Channel. This channel works in tandem with the N-Channel to minimize drain-to-source leakage and minimize the effects of electrostatic discharge in the device. The P-Channel also acts as a current limiter, preventing the device from drawing more than a certain amount of current.
Conclusion
The SQP10250E_GE3 is a single N-Channel enhancement-mode, field effect transistor suitable for use in a variety of applications. With a wide range of features, the SQP10250E_GE3 is highly versatile and is capable of providing superior performance in power management, high-speed switching, automotive, and other industrial and consumer applications. Furthermore, its working principle helps to ensure that the device is reliable and highly efficient in all its applications.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
SQP10250E_GE3 | Vishay Silic... | 2.34 $ | 1000 | MOSFET N-CH 250V TO-220AB... |
SQP120N10-3M8_GE3 | Vishay Silic... | -- | 200 | MOSFET N-CH 100V 120A TO2... |
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SQP10AJB-0R11 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL110 mOhms... |
SQP10AJB-0R12 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL120 mOhms... |
SQP10AJB-0R13 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL130 mOhms... |
SQP10AJB-0R15 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL150 mOhms... |
SQP10AJB-0R16 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL160 mOhms... |
SQP10AJB-0R18 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL180 mOhms... |
SQP10AJB-0R2 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL200 mOhms... |
SQP10AJB-0R22 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL220 mOhms... |
SQP10AJB-0R24 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL240 mOhms... |
SQP10AJB-0R27 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL270 mOhms... |
SQP10AJB-0R3 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL300 mOhms... |
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SQP10AJB-0R39 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL390 mOhms... |
SQP10AJB-0R43 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL430 mOhms... |
SQP10AJB-0R47 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL470 mOhms... |
SQP10AJB-0R51 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL510 mOhms... |
SQP10AJB-0R56 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL560 mOhms... |
SQP10AJB-0R62 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL620 mOhms... |
SQP10AJB-0R68 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL680 mOhms... |
SQP10AJB-0R75 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL750 mOhms... |
SQP10AJB-0R82 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL820 mOhms... |
SQP10AJB-0R91 | Yageo | 0.09 $ | 1000 | RES 10W 5% AXIAL910 mOhms... |
SQP10AJB-2R1 | Yageo | 0.07 $ | 1000 | RES 2.1 OHM 10W 5% AXIAL2... |
SQP10AJB-100K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL100 kOhms... |
SQP10AJB-10K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL10 kOhms ... |
SQP10AJB-11K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL11 kOhms ... |
SQP10AJB-12K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL12 kOhms ... |
SQP10AJB-13K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL13 kOhms ... |
SQP10AJB-15K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL15 kOhms ... |
SQP10AJB-16K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL16 kOhms ... |
SQP10AJB-18K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL18 kOhms ... |
SQP10AJB-20K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL20 kOhms ... |
SQP10AJB-22K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL22 kOhms ... |
SQP10AJB-24K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL24 kOhms ... |
SQP10AJB-27K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL27 kOhms ... |
SQP10AJB-30K | Yageo | 0.07 $ | 1000 | RES 10W 5% AXIAL30 kOhms ... |
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