MMJT350T1G Allicdata Electronics
Allicdata Part #:

MMJT350T1GOSTR-ND

Manufacturer Part#:

MMJT350T1G

Price: $ 0.18
Product Category:

Discrete Semiconductor Products

Manufacturer: ON Semiconductor
Short Description: TRANS PNP 300V 0.5A SOT-223
More Detail: Bipolar (BJT) Transistor PNP 300V 500mA 650mW Sur...
DataSheet: MMJT350T1G datasheetMMJT350T1G Datasheet/PDF
Quantity: 5000
1000 +: $ 0.15957
2000 +: $ 0.14549
5000 +: $ 0.13611
10000 +: $ 0.12672
25000 +: $ 0.12516
Stock 5000Can Ship Immediately
$ 0.18
Specifications
Series: --
Packaging: Tape & Reel (TR) 
Part Status: Active
Transistor Type: PNP
Current - Collector (Ic) (Max): 500mA
Voltage - Collector Emitter Breakdown (Max): 300V
Vce Saturation (Max) @ Ib, Ic: --
Current - Collector Cutoff (Max): 100nA (ICBO)
DC Current Gain (hFE) (Min) @ Ic, Vce: 30 @ 50mA, 10V
Power - Max: 650mW
Frequency - Transition: --
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: MMJT350
Description

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The MMJT350T1G is a single Bipolar Junction Transistor (BJT) that is designed for use in a variety of applications. The device is particularly suited for high-speed switching applications such as power MOSFETs, as well as for use in amplifier stages. The single-channel transistor also features excellent gain, high current gain, and very low power dissipation.

The MMJT350T1G is a general purpose, silicon single NPN transistor with a maximum collector current of 350mA. The package of the MMJT350T1G is a TO-220FD style. The device features a flat gain-bandwidth product of 3GHz, as well as aDC current gain of 350. Other characteristics of the MMJT350T1G include a maximum collector emitter voltage rating of 60V. The MMJT350T1G also features a maximum collector dissipation of 625mW.

As a single bipolar junction transistor, the MMJT350T1G device contains three layers of a semiconductor material. In a BJT, two layers of semiconductor material, either two slices of silicon, are connected together. These two layers will form two P-N junctions, or gates, that are connected to the Emitter (E) and Base (B) terminals of the transistor. A third layer, or collector, is also connected to the Base terminal. This third layer of semiconductor material will form a third P-N junction with the Base layer, forming the Collector-Base junction.

The transistor works by allowing the current to flow from the Base to the Emitter which is then amplified by the Collector. This works due to the transistor’s three layers of semiconductor material forming the three P-N junctions. When a voltage is applied to the Base and Emitter, current flows through the Base-Emitter junction and is amplified by the Collector-Base junction. This is known as the transistor’s active region and will allow the current to pass through.

Using this principle and its characteristics, the MMJT350T1G can be used in a wide range of applications. Due to its very low power dissipation and high current gain, the device is well-suited for use in power MOSFET circuits. It is also great for use in amplifier stages due to its flat gain-bandwidth product. As with all BJTs, the device can also be used in logic circuits as well as for switching applications.

The MMJT350T1G is a great all-around solution for many applications. It has a variety of features that make it an excellent choice for high speed switching, power MOSFETs, and amplifier circuits. The device is also low cost, making it a very attractive option for most designers.

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

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