KSH2955TM Allicdata Electronics
Allicdata Part #:

KSH2955TMTR-ND

Manufacturer Part#:

KSH2955TM

Price: $ 0.00
Product Category:

Discrete Semiconductor Products

Manufacturer: ON Semiconductor
Short Description: TRANS PNP 60V 10A DPAK
More Detail: Bipolar (BJT) Transistor PNP 60V 10A 2MHz 1.75W Su...
DataSheet: KSH2955TM datasheetKSH2955TM Datasheet/PDF
Quantity: 1000
Stock 1000Can Ship Immediately
Specifications
Series: --
Packaging: Tape & Reel (TR) 
Part Status: Active
Transistor Type: PNP
Current - Collector (Ic) (Max): 10A
Voltage - Collector Emitter Breakdown (Max): 60V
Vce Saturation (Max) @ Ib, Ic: 8V @ 3.3A, 10A
Current - Collector Cutoff (Max): 50µA
DC Current Gain (hFE) (Min) @ Ic, Vce: 20 @ 4A, 4V
Power - Max: 1.75W
Frequency - Transition: 2MHz
Operating Temperature: 150°C (TJ)
Mounting Type: Surface Mount
Package / Case: TO-252-3, DPak (2 Leads + Tab), SC-63
Supplier Device Package: D-Pak
Base Part Number: KSH2955
Description

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KSH2955TM is a type of single bipolar junction transistor (BJT). As an electrical switch, a BJT can be utilized to control current flow between two terminals, one denoted as the base, and the other as the collector and emitter. Through applying a small amount of current to the base, a larger amount of current can be shifted between the other terminals. This is a result of the BJT’s gain - the ratio of current flow from the collector to the base compared to the current from the base to the emitter.

The KSH2955TM has a wide range of applications, including in mobility amplifiers, photonics, high-performance RF systems, communications, and automotive electronics. It can also be used in applications with higher breakdown voltages. In these applications, the transistor can be used to create higher power gains over a wider range of frequencies.

The working principle of the KSH2955TM is based on the operation of a diode junction and current flow. When current is applied to the base terminal, it creates a potential difference between the collector and emitter of the BJT. This creates a base-emitter voltage which, when greater than the breakdown voltage of the BJT, opens a small “gate” through which current can flow from the collector to the emitter. Due to the BJT’s gain, a greater current flows from the collector than from the base to the emitter.

KSH2955TM has an NPN device, which is a combination of two PN junctions, of which one interconnects the base and collector and the other interconnects the base and emitter. The NPN BJT is polarized in such a way that the base is negative with respect to the emitter, while the collector is positive relative to the emitter. As current is fed through the base, it charges up the base collecting layer. This causes electrons to be repelled from the base and attracted to the collector. As the repulsive force is greater than the attractive force, current starts flowing from the collector to the emitter. This is how the KSH2955TM amplifies an input signal.

KSH2955TM has a wide range of applications, including in mobility amplifiers, photonics, high-performance RF systems, communications, and automotive electronics. It is also suitable for use with other BJT, diode, and resistor components as part of complex circuits. Other beneficial features of the BJT include low power dissipation, high switching speed, and high current gain.

In conclusion, KSH2955TM is a single bipolar transistor that is suitable for use in a wide range of applications. Its working principle is based on the operation of a diode junction and current flow and it is capable of amplifying an input signal with a high current gain. The device is applicable in many industries and has additional features such as low power dissipation, high switching speed, and high current gain.

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

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