2N5087G Allicdata Electronics
Allicdata Part #:

2N5087GOS-ND

Manufacturer Part#:

2N5087G

Price: $ 0.00
Product Category:

Discrete Semiconductor Products

Manufacturer: ON Semiconductor
Short Description: TRANS PNP 50V 0.05A TO-92
More Detail: Bipolar (BJT) Transistor PNP 50V 50mA 40MHz 625mW ...
DataSheet: 2N5087G datasheet2N5087G Datasheet/PDF
Quantity: 1000
Stock 1000Can Ship Immediately
Specifications
Series: --
Packaging: Bulk 
Part Status: Obsolete
Transistor Type: PNP
Current - Collector (Ic) (Max): 50mA
Voltage - Collector Emitter Breakdown (Max): 50V
Vce Saturation (Max) @ Ib, Ic: 300mV @ 1mA, 10mA
Current - Collector Cutoff (Max): 50nA (ICBO)
DC Current Gain (hFE) (Min) @ Ic, Vce: 250 @ 100µA, 5V
Power - Max: 625mW
Frequency - Transition: 40MHz
Operating Temperature: -55°C ~ 150°C (TJ)
Mounting Type: Through Hole
Package / Case: TO-226-3, TO-92-3 (TO-226AA)
Supplier Device Package: TO-92-3
Base Part Number: 2N5087
Description

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The 2N5087G is a single Bipolar Junction Transistor (BJT). It is typically used in a variety of electronic applications. This device is manufactured by semiconductor material in a planar structure known as a die. Its usage as an amplifier and switch is possible due to its relatively high current gain when operating in the common Emitter configuration and its ability to switch currents between a collector and an emitter. Other features include low-noise operation and a low-power consumption design.

The 2N5087G is a NPN transistor, where NPN stands for the three layers of semiconductor materials that make up the device. The base of the transistor houses the N material, while the collector and emitter both contain P materials. To ensure stability while in operation, the layers are appropriately separated by doping. Between each layer is also a junction, which allows for a flow of electrons from one layer to the other.

During operation, the transistor acts as a current amplifier, as well as a switch for potential differences. To begin, the base of the NPN transistor needs to be biased with a voltage. This allows for a flow of current from the Collector to the Emitter, and creates a gain known as “hfe”. The hfe is the amount of voltage that can be amplified for each unit of current going through the transistor. For the 2N5087G, this current gain ranges from 75 to 150, depending on the conditions of the circuit.

The current that flows through the circuit is also known as collector current and is derived from the current flowing through the base. This current flows through the transistor as a result of the high resistivity of the P material in the base layer. The collector current is typically much greater than the current that flows through the base, making the transistor an ideal amplifier. This is because the current gain can be controlled by changing the bias current of the transistor.

Switching is also possible due to the transistor’s ability to switch between its two states. A low current will cause the transistor to switch off and halt current flow. A high current on the other hand, can cause the transistor to switch on and allow current through. This is possible due to the resistivity of the P region in the base layer. When the current is high enough, a potential difference will form across the transistor, allowing for current flow from the collector to the emitter.

The 2N5087G is thus an ideal device for use in amplifiers and switches. Its low-noise operation and low-power consumption further enhance its versatility for such applications. Additionally, it features a built-in ESD protection to shield it against static discharges. This feature is particularly useful for its intended applications, as it allows the device to remain reliable and stable in a variety of conditions.

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

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