BFR106E6327HTSA1 Allicdata Electronics

BFR106E6327HTSA1 Discrete Semiconductor Products

Allicdata Part #:

BFR106E6327HTSA1TR-ND

Manufacturer Part#:

BFR106E6327HTSA1

Price: $ 0.08
Product Category:

Discrete Semiconductor Products

Manufacturer: Infineon Technologies
Short Description: TRANSISTOR RF NPN 15V SOT-23
More Detail: RF Transistor NPN 15V 210mA 5GHz 700mW Surface Mou...
DataSheet: BFR106E6327HTSA1 datasheetBFR106E6327HTSA1 Datasheet/PDF
Quantity: 1000
3000 +: $ 0.06809
6000 +: $ 0.06396
15000 +: $ 0.05984
30000 +: $ 0.05489
75000 +: $ 0.05282
Stock 1000Can Ship Immediately
$ 0.08
Specifications
Series: --
Packaging: Tape & Reel (TR) 
Part Status: Active
Transistor Type: NPN
Voltage - Collector Emitter Breakdown (Max): 15V
Frequency - Transition: 5GHz
Noise Figure (dB Typ @ f): 1.8dB ~ 3dB @ 900MHz ~ 1.8Ghz
Gain: 8.5dB ~ 13dB
Power - Max: 700mW
DC Current Gain (hFE) (Min) @ Ic, Vce: 70 @ 70mA, 8V
Current - Collector (Ic) (Max): 210mA
Operating Temperature: 150°C (TJ)
Mounting Type: Surface Mount
Package / Case: TO-236-3, SC-59, SOT-23-3
Supplier Device Package: SOT-23-3
Base Part Number: BFR106
Description

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The BFR106E6327HTSA1 is a single NPN transistor used in a variety of different applications, typically as an amplifier or oscillator. It is categorised as a transistor type known as a Bipolar Junction Transistor (BJT) - Radio Frequency, abbreviated RF. This type of transistor typically operates at higher frequencies, and is used in communications, radio and digital electronics.

This transistor is designed to handle approximately 5 watts and has a maximum current gain of 300, with a minimum of 10 (it has a beta range of 10 to 300). With a power gain of 5 watts, it can be used as a high-frequency amplifier in a range of different applications such as radio and terrestrial communication, RF amplifiers and oscillators, medical electronics, and base station amplifiers.

The BFR106E6327HTSA1 works on the concept of a PN junction. A PN junction is a connection between two different types of semiconductor materials, namely P type and N type. The PN junction can be thought of as a diode, in that it allows current to flow in only one direction. The PN junction can also be thought of as a transistor, in that it can amplify a weak signal.

The way that a PN junction works is by creating a depletion region in the junction. This happens when there is an electric current flowing in one direction through the junction, creating a thin layer of electrostatic field. This thin layer of electrostatic field acts as an insulator, blocking any current from flowing through the junction in the opposite direction. As such, this creates a one way conduction of electrons and is known as the diode effect.

The BFR106E6327HTSA1 works by using the same concept of a PN junction. It consists of a N-type and P-type region where a current flowing in one direction through the junction creates a thin layer of electrostatic field. This thin layer of electrostatic field acts as an insulator, blocking any current from flowing in the reverse direction. This "diode effect" is what allows the transistor to work as an amplifier or oscillator.

The BFR106E6327HTSA1 is also capable of producing an oscillatory action by means of what is known as the "transconductance bias" configuration. This configuration allows for collections of signals to be combined to form complex signals such as a sinusoidal waveform. In this configuraiton, two collector currents (IC1 and IC2) are combined to form a single output current. The two collector currents are generated by the application of a bias voltage to the base terminal of the transistor.

In summary, the BFR106E6327HTSA1 transistor is a Radio Frequency (RF) Bipolar Junction Transistor (BJT) designed to handle approximately 5 watts and has a maximum current gain of 300, with a minimum of 10. It can be used as a high frequency amplifier in radio and terrestrial communication, RF amplifiers and oscillators, medical electronics, and base station amplifiers. It works on the principle of the PN junction, in which a current flowing in one direction through the junction creates an electrostatic field that can be used as an insulator. Additionally, it is capable of producing an oscillatory action by means of a transconductance bias configuration.

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

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