Allicdata Part #: | 2N4401RLRM-ND |
Manufacturer Part#: |
2N4401RLRM |
Price: | $ 0.00 |
Product Category: | Discrete Semiconductor Products |
Manufacturer: | ON Semiconductor |
Short Description: | TRANS NPN 40V 0.6A TO-92 |
More Detail: | Bipolar (BJT) Transistor NPN 40V 600mA 250MHz 625m... |
DataSheet: | 2N4401RLRM Datasheet/PDF |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | -- |
Packaging: | Tape & Box (TB) |
Part Status: | Obsolete |
Transistor Type: | NPN |
Current - Collector (Ic) (Max): | 600mA |
Voltage - Collector Emitter Breakdown (Max): | 40V |
Vce Saturation (Max) @ Ib, Ic: | 750mV @ 50mA, 500mA |
Current - Collector Cutoff (Max): | -- |
DC Current Gain (hFE) (Min) @ Ic, Vce: | 100 @ 150mA, 1V |
Power - Max: | 625mW |
Frequency - Transition: | 250MHz |
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: | 2N4401 |
Due to market price fluctuations, if you need to purchase or consult the price. You can contact us or emial to us: sales@allicdata.com
The 2N4401RLRM is a NPN Silicon RF Transistor that is normally used as an amplification and switching device. It is widely used in different fields such as telecommunications, IT, power supplies and mobile phones. It is a bipolar junction transistor (BJT) constructed in a plastic package with multiple connectors to provide the user with an efficient solution. The transistor consists of a base, emitter, and collector connection giving three terminals, is used for both amplifying and switching applications.
The 2N4401RLRM has an operating frequency up to 500 MHz, collector current up to 0.8A, and power dissipation up to 0.75W. The transistor has two active zones, an amplification zone and a saturation zone that work together when the transistor is in operation. In the amplification zone, the transistor has a high linear current gain and remains slightly open. In this zone, the transistor act as an amplifier where a small current at either the base or collector is amplified at the output. On the other hand, the saturation zone is an area where the transistor is completely open and completely conducts current. This is where the transistor works as a switch and one terminal is activated while the other is deactivated.
The transistor has different components that work together in order to provide the stability and speed needed to obtain the desired current and voltage characteristics. In addition, the transistor also has a base-emitter junction that is responsible for controlling the flow of current between the collector and the emitter in a feedback loop. This process is governed by thermionic emission and electrostatic field coupling of warm electrons from the emitter, as well as conduction from the collector, which is mainly responsible for the flow of current.
The internal components of the 2N4401RLRM consist of a base-to-emitter junction, collector-to-base junction, and a diode junction between the collector and the emitter. The Collector-to-base junction adds gain to the device and the base-emitter junction adds stability, both of these characteristics help to maintain a stable operation. The diode junction promotes electron emission from the collector to the base, thus controlling the current.
The 2N4401RLRM is used in many applications such as; radio frequency amplifiers, oscillators, switch circuits and audio amplifiers, among others. Generally, the 2N4401RLRM has a wide variety of uses, due to its robust construction, operating frequency, and its low voltage and temperature coefficients. Also, the 2N4401RLRM has a breakdown voltage of around 30V and can handle up to 400mA of current, making it suitable for high power applications. Furthermore, due to its high input impedances and its low noise characteristics, the 2N4401RLRM is often used as a pre-amplifier, a frequency multiplier, and modulator circuits.
Overall, the 2N4401RLRM is an ideal choice for a wide range of applications due to its robust construction, operating frequency, low-noise characteristics, and low-temperature coefficients. It is widely used in telecommunications, power supplies, IT, and mobile phones. Thus, the 2N4401RLRM can be used in a wide range of applications including, radio frequency amplifiers, oscillators, switch circuits and audio amplifiers among others.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
2N4401RLRA | ON Semicondu... | -- | 1000 | TRANS NPN 40V 0.6A TO92Bi... |
2N4403RLRA | ON Semicondu... | -- | 1000 | TRANS PNP 40V 0.6A TO92Bi... |
2N4401T93 | ROHM Semicon... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4403T93 | ROHM Semicon... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4401,116 | NXP USA Inc | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO92Bi... |
2N4401G | ON Semicondu... | -- | 3138 | TRANS NPN 40V 0.6A TO-92B... |
2N4401RLRM | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4401RLRMG | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4401RLRPG | ON Semicondu... | -- | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4403G | ON Semicondu... | -- | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4403RL | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4403RLG | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4403RLRM | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4403RLRMG | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4403RLRP | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4403RLRPG | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4401RLRAG | ON Semicondu... | -- | 1000 | TRANS NPN 40V 0.6A TO92Bi... |
2N4403RLRAG | ON Semicondu... | -- | 1000 | TRANS PNP 40V 0.6A TO92Bi... |
2N4403_D11Z | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4400TA | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4400TF | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4400TFR | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4401NLBU | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4402TA | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4402TF | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4402TFR | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4403NLBU | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
2N4400_D81Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4400_S00Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4400TAR | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4401_D11Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4401_D81Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4401_J05Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4401_J18Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4401_J25Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4401_J60Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4401_J61Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4401_S00Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
2N4402TAR | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
GENERAL-PURPOSE TRANSISTORBipolar (BJT) ...
TRANS PNP DARL 30A 120V DIEBipolar (BJT)...
TRANS PNP DARLINGTON DIEBipolar (BJT) Tr...
TRANS GENERAL PURPOSE TO-218Bipolar (BJT...
TRANS PNP 140V 1ABipolar (BJT) Transisto...
TRANS NPN 700V 3A I2PAKBipolar (BJT) Tra...