PN2907ARLRAG Allicdata Electronics

PN2907ARLRAG Discrete Semiconductor Products

Allicdata Part #:

PN2907ARLRAGOSTR-ND

Manufacturer Part#:

PN2907ARLRAG

Price: $ 0.00
Product Category:

Discrete Semiconductor Products

Manufacturer: ON Semiconductor
Short Description: TRANS PNP 60V 0.6A TO92
More Detail: Bipolar (BJT) Transistor PNP 60V 600mA 200MHz 625m...
DataSheet: PN2907ARLRAG datasheetPN2907ARLRAG Datasheet/PDF
Quantity: 1000
1 +: 0.00000
Stock 1000Can Ship Immediately
$ 0
Specifications
Series: --
Packaging: Tape & Reel (TR) 
Part Status: Obsolete
Transistor Type: PNP
Current - Collector (Ic) (Max): 600mA
Voltage - Collector Emitter Breakdown (Max): 60V
Vce Saturation (Max) @ Ib, Ic: 1.6V @ 50mA, 500mA
Current - Collector Cutoff (Max): 10nA (ICBO)
DC Current Gain (hFE) (Min) @ Ic, Vce: 100 @ 150mA, 10V
Power - Max: 625mW
Frequency - Transition: 200MHz
Operating Temperature: -55°C ~ 150°C (TJ)
Mounting Type: Through Hole
Package / Case: TO-226-3, TO-92-3 (TO-226AA) (Formed Leads)
Supplier Device Package: TO-92-3
Base Part Number: PN2907A
Description

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The PN2907ARLRAG is a type of bipolar junction transistor (BJT). As a single BJT transistor, the active region of the device is constituted by a p-type base layer sandwiched between n-type emitter and collector regions. Because of its ability to amplify electrical signals, the PN2907ARLRAG is used in a plethora of applications.

The PN2907ARLRAG is a NPN type of bipolar junction transistor, with a small signal current gain of up to 75 and a maximum current handling capability of 500mA. It has a low saturation voltage of 0.2V and a base-emitter voltage of 1.2 V. Due to its low-power consumption, it is especially suitable for small portable applications and finds typical applications in switching circuits, small signal amplification stages, inverters, and oscillator circuits.

The working principle of the PN2907ARLRAG begins by turning it into an active state by supplying positive current to its base terminal. This positive voltage helps to biase the transistor within its active region. This allows hole-electron pairs, or carriers, to flow from the emitter to the collector region. When the transistor is forward biase the collector-emitter current IC is proportional to the base current IB through the small signal current gain (beta) of the device. The current gain beta is defined as IC divided by IB for a given transistor. Thus, for someone to predict current gain, the base current has to be known.

In addition to its use in switching applications, the PN2907ARLRAG can also be employed in amplifying small signals. An amplifier is a circuit that takes an input signal and makes it larger at the output while introducing some degree of distortion. The PN2907ARLRAG can act as both an amplifier and a switch, depending on the operating conditions. When the device is used as an amplifier the base current is once again critical and is controlled by the input signal voltage. As the input voltage increases an increased current flows from the emitter to the collector thus amplifying the input signal. The important parameters for designing an amplifier with the PN2907ARLRAG are the base-emitter voltage and the base-collector voltage.

Apart from amplifying small signals, the PN2907ARLRAG is also used in oscillator circuits. Oscillators are used to generate periodic waveforms such as square waves, sine waves, and saw tooth waves and are a key circuit block in many electronic circuitry. The PN2907ARLRAG is advantageous in oscillator applications since its current gain characteristics can be exploited to generate oscillations. To generate the oscillations, the PN2907ARLRAG is biased slightly at the edge of the saturation and active region. When the output voltage varies slightly above and below the saturation region at a certain frequency, the transistor will start oscillating. This frequency is then considered as the oscillator\'s frequency.

In conclusion, the PN2907ARLRAG is a transistor with a small signal current gain of up to 75 and a maximum current handling capability of 500mA. Its low saturation voltage of 0.2V and a base-emitter voltage of 1.2V makes it suitable for many applications such as switching circuits, small signal amplification stages, inverters, and oscillator circuits. Its working principle involves biasing the transistor within its active region and using the current gain characteristics to amplify small signals or oscillate.

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

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