2SC3906KT146S Allicdata Electronics
Allicdata Part #:

2SC3906KT146STR-ND

Manufacturer Part#:

2SC3906KT146S

Price: $ 0.08
Product Category:

Discrete Semiconductor Products

Manufacturer: ROHM Semiconductor
Short Description: TRANS NPN 120V 0.05A SOT-346
More Detail: Bipolar (BJT) Transistor NPN 120V 50mA 140MHz 200m...
DataSheet: 2SC3906KT146S datasheet2SC3906KT146S Datasheet/PDF
Quantity: 3000
1 +: $ 0.08000
10 +: $ 0.07760
100 +: $ 0.07600
1000 +: $ 0.07440
10000 +: $ 0.07200
Stock 3000Can Ship Immediately
$ 0.08
Specifications
Series: --
Packaging: Tape & Reel (TR) 
Part Status: Active
Transistor Type: NPN
Current - Collector (Ic) (Max): 50mA
Voltage - Collector Emitter Breakdown (Max): 120V
Vce Saturation (Max) @ Ib, Ic: 500mV @ 1mA, 10mA
Current - Collector Cutoff (Max): 500nA (ICBO)
DC Current Gain (hFE) (Min) @ Ic, Vce: 180 @ 2mA, 6V
Power - Max: 200mW
Frequency - Transition: 140MHz
Operating Temperature: 150°C (TJ)
Mounting Type: Surface Mount
Package / Case: TO-236-3, SC-59, SOT-23-3
Supplier Device Package: SMT3
Base Part Number: 2SC3906
Description

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2SC3906KT146S BJT is one of the most commonly used transistors in the market. It is a single general purpose low frequency bipolar junction transistor, with a maximum collector current rating of 0.6 amp. It can be used as an amplifier, oscillator, or switch.

When using this device, the collector is connected to the positive voltage of the circuit, the base is connected to the negative voltage of the circuit, and the emitter is connected to the load. This basic configuration can be used to amplify signals, or switch a large current on and off, depending on the signal received at the base.

The primary application fields of 2SC3906KT146S BJT is in the low frequency amplifying and switching circuits. It is used in applications such as audio amplifiers, portable radios, telephone receivers, converters, and motor drives. It is also used in logic gates and other digital circuit applications that require high-speed switching operations.

The working principle of the BJT is quite simple and relies on the effect of exchanging charge carriers between the base and emitter terminals. When no base voltage is applied, the collector current is zero since the PN junction at the base-emitter junction is reverse-biased. When base voltage is applied, majority carriers are injected into the base, and they will then be drawn towards the collector, causing a current to flow in the collector circuit. This current is known as the collector current.

The working of 2SC3906KT146S BJT can be explained as follows: The voltage applied to the base (VBE) causes some holes to be injected into the base region. These holes start to diffuse through the base to the collector region. As the base-emitter voltage increases, more holes are injected and can be collected at the collector junction. The injected holes create a net negative charge in the collector region and give rise to an electric field in the base-emitter region of the transistor, driving holes away from the base terminal. This electric field strengthens and the collector current increases, resulting in the transistor\'s gain.

To sum up, 2SC3906KT146S BJT is a single general purpose low frequency bipolar junction transistor with a maximum collector current rating of 0.6 amp. It is mainly used in low frequency amplifying and switching circuits, such as audio amplifiers, telephone receivers, converters, and motor drives. Its working principle relies on the effect of exchanging charge carriers between the base and emitter terminals, when a voltage is applied to the base. It is a reliable, efficient, and cost-effective solution for the mentioned applications.

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

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