NJT4030PT1G Allicdata Electronics

NJT4030PT1G Discrete Semiconductor Products

Allicdata Part #:

NJT4030PT1GOSTR-ND

Manufacturer Part#:

NJT4030PT1G

Price: $ 0.11
Product Category:

Discrete Semiconductor Products

Manufacturer: ON Semiconductor
Short Description: TRANS PNP 40V 3A SOT-223
More Detail: Bipolar (BJT) Transistor PNP 40V 3A 160MHz 2W Surf...
DataSheet: NJT4030PT1G datasheetNJT4030PT1G Datasheet/PDF
Quantity: 18000
1000 +: $ 0.10252
2000 +: $ 0.09398
5000 +: $ 0.08828
10000 +: $ 0.08259
25000 +: $ 0.07594
Stock 18000Can Ship Immediately
$ 0.11
Specifications
Series: --
Packaging: Tape & Reel (TR) 
Part Status: Active
Transistor Type: PNP
Current - Collector (Ic) (Max): 3A
Voltage - Collector Emitter Breakdown (Max): 40V
Vce Saturation (Max) @ Ib, Ic: 500mV @ 300mA, 3A
Current - Collector Cutoff (Max): 100nA (ICBO)
DC Current Gain (hFE) (Min) @ Ic, Vce: 200 @ 1A, 1V
Power - Max: 2W
Frequency - Transition: 160MHz
Operating Temperature: -55°C ~ 150°C (TJ)
Mounting Type: Surface Mount
Package / Case: TO-261-4, TO-261AA
Supplier Device Package: SOT-223
Base Part Number: NJT4030
Description

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NJT4030PT1G Application Field and Working Principle

NJT4030PT1G is a type of bipolar transistor, also known as a Bipolar Junction Transistor (BJT). The NJT4030PT1G is a low-power two-terminal BJT made of silicon, with a switching speed of 0.1 microsecond and a voltage drop of 0.60V. It is typically used in applications involving high speed switching, such as in telecommunication and computer circuits.

The NJT4030PT1G has a collector-emitter voltage of 30 V with a collector current of 0.2 A. It also has a maximum power dissipation of 0.1 W and an insulated gate voltage of -20 V. The NJT4030PT1G is typically used in RF and IF circuits, as well as in high-speed switching applications. It is also used in circuits that require high switching speed and low power dissipation.

Working Principle

The NJT4030PT1G operates on the principle of bipolar junction transistors (BJT). It is a two-terminal device consisting of a P-type and N-type semiconductor material. The two materials form two regions, the base and the collector. The base is the middle region between the collector and the emitter, and the collector is the outermost region that makes contact with the emitter. A voltage applied to the base creates a current flow between the P-type region and the N-type material. This current flow creates a voltage drop across the collector-emitter junction.

How it works

The NJT4030PT1G operates in three states. The OFF state occurs when the base is open and no current can flow through the transistor. The ON state is where the base voltage is greater than the cutoff voltage, thus allowing current flow from the collector to the emitter. The saturation state is when the base-emitter junction is forward biased and the collector-emitter junction is reverse biased, resulting in current flow from the collector to the emitter.

The NJT4030PT1G is an NPN transistor, so the P-type and N-type materials form a sandwich structure, with the collector-base junction at the base, the emitter-base junction at the collector, and the emitter-collector junction at the emitter. When a voltage is applied to the base, the electrons are attracted to the P-type material, leaving the N-type material positively charged. This creates an internal electric field and sets up a current flow between the collector and emitter. This current flow controls the output of the transistor.

Applications

The NJT4030PT1G is used in a variety of applications, primarily involving high-speed switching. Some of these applications include:

  • Telecommunication systems
  • Computer systems
  • Logic circuits
  • Light-emitting diodes
  • Microprocessor systems
  • Voltage regulation

The NJT4030PT1G is also used in RF and IF circuits, as well as in power converter circuits. In addition, it can be used to amplify small signals, and it is often used in switching power supplies.

Conclusion

The NJT4030PT1G is a low-power, two-terminal bipolar transistor made of silicon, with a switching speed of 0.1 microsecond and a voltage drop of 0.60V. It is used in high-speed switching applications, such as in telecommunication and computer systems, logic circuits, and microprocessor systems. Additionally, it is used in RF and IF circuits, as well as in power converter circuits, and it is often used in switching power supplies.

The specific data is subject to PDF, and the above content is for reference

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