ZTX853STOA Allicdata Electronics
Allicdata Part #:

ZTX853STOA-ND

Manufacturer Part#:

ZTX853STOA

Price: $ 0.00
Product Category:

Discrete Semiconductor Products

Manufacturer: Diodes Incorporated
Short Description: TRANS NPN 100V 4A E-LINE
More Detail: Bipolar (BJT) Transistor NPN 100V 4A 130MHz 1.2W T...
DataSheet: ZTX853STOA datasheetZTX853STOA Datasheet/PDF
Quantity: 1000
1 +: 0.00000
Stock 1000Can Ship Immediately
$ 0
Specifications
Series: --
Packaging: Tape & Reel (TR) 
Part Status: Obsolete
Transistor Type: NPN
Current - Collector (Ic) (Max): 4A
Voltage - Collector Emitter Breakdown (Max): 100V
Vce Saturation (Max) @ Ib, Ic: 200mV @ 400mA, 4A
Current - Collector Cutoff (Max): 50nA (ICBO)
DC Current Gain (hFE) (Min) @ Ic, Vce: 100 @ 2A, 2V
Power - Max: 1.2W
Frequency - Transition: 130MHz
Operating Temperature: -55°C ~ 200°C (TJ)
Mounting Type: Through Hole
Package / Case: E-Line-3
Supplier Device Package: E-Line (TO-92 compatible)
Base Part Number: ZTX853
Description

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ZTX853STOA Application Field and Working Principle

The ZTX853STOA transistor is a type of bipolar junction transistor (BJT) known as a single. It operates at voltages of 10 V, is a discrete device, and is suitable for use in a wide range of amplifying and switching applications. The ZTX853STOA has a maximum power dissipation of 500 mW and is suitable for voltage regulation and interface circuitry.

A bipolar junction transistor (BJT) is one of the most commonly used components in electronic circuit design. It is composed of two base layers and a two base-collector barrier layers, and it works by transducing changes of small electronic currents into much large electronic current and vice versa. BJTs often incorporate three "junctions" of semiconductor material: the base-emitter junction, the base-collector junction, and the collector-emitter junction. Each of these junctions plays an important role in BJT operation.

The ZTX853STOA is designed to work in a common emitter configuration. In this configuration, current flows from the collector, through the base, and then into the emitter. The base-emitter junction is forward-biased while the base-collector junction is reverse biased. The amount of voltage drop across the collector-emitter junction determines the amount of current that is allowed to flow through the transistor.

As the base-emitter junction is forward-biased, it allows a proportion of the voltage applied across the collector-emitter circuit to appear across the base-emitter circuit. The proportion of voltage drop is then determined by the transistor\'s Beta (β) rating. In the ZTX853STOA, the Beta rating is 100, meaning that for a 10 V voltage applied across the collector-emitter circuit, only 100 mV would appear across the base-emitter junction.

This allows for the current in the collector to be easily controlled. By varying the resistors in the base-emitter circuit, the amount of current that is allowed to flow through the base-emitter junction can be adjusted and the amount of collector current that is allowed to flow through the transistor can be increased or decreased.

The ZTX853STOA has a high gain-bandwidth ratio, has low collector-emitter saturation voltage, and can handle very high switching frequencies. This makes it well-suited for a wide range of applications, such as voltage regulation, interface circuitry, and as a switch.

In summary, the ZTX853STOA is a single bipolar junction transistor (BJT) that operates at voltages of 10V and has a maximum power dissipation of 500 mW. It has a Beta rating of 100 and works in a common emitter configuration. It has a high gain-bandwidth ratio, low collector-emitter saturation voltage, and can handle very high switching frequencies, making it well-suited for a variety of amplifying and switching applications.

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

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