2N4410 Discrete Semiconductor Products |
|
| Allicdata Part #: | 2N4410CS-ND |
| Manufacturer Part#: |
2N4410 |
| Price: | $ 0.00 |
| Product Category: | Discrete Semiconductor Products |
| Manufacturer: | Central Semiconductor Corp |
| Short Description: | TRANS NPN 80V 0.25A TO-92 |
| More Detail: | Bipolar (BJT) Transistor NPN 80V 250mA 300MHz 625m... |
| DataSheet: | 2N4410 Datasheet/PDF |
| Quantity: | 1000 |
| 1 +: | 0.00000 |
| Series: | -- |
| Packaging: | Bulk |
| Part Status: | Active |
| Transistor Type: | NPN |
| Current - Collector (Ic) (Max): | 250mA |
| Voltage - Collector Emitter Breakdown (Max): | 80V |
| Vce Saturation (Max) @ Ib, Ic: | 200mV @ 100µA, 1mA |
| Current - Collector Cutoff (Max): | 10nA (ICBO) |
| DC Current Gain (hFE) (Min) @ Ic, Vce: | 60 @ 10mA, 1V |
| Power - Max: | 625mW |
| Frequency - Transition: | 300MHz |
| Operating Temperature: | -65°C ~ 150°C (TJ) |
| Mounting Type: | Through Hole |
| Package / Case: | TO-226-3, TO-92-3 (TO-226AA) |
| Supplier Device Package: | TO-92 |
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
2N4410 is a medium-power NPN silicon transistor commonly used for a variety of applications.
The 2N4410 is designed to be used in low to medium frequency linear circuits and also in medium to high frequency low-noise circuits. It has an optimal speed/power ratio, making it an excellent choice for medium power general-purpose applications. This transistor is also commonly used for audio amplifying applications and should be used within its specified power dissipation limits. The transistor comes in two different versions: the general purpose version 2N4410 and the high-gain version 2N4410G. The difference between the two is the collector current in mA.
The 2N4410 is a single bipolar transistor, which means it has three terminals: emitter, collector and base. The collector terminal is designated as C, the base terminal as B and the emitter terminal as E. The terminals have a maximum rating for collector current (Ic), collector-emitter voltage (Vce) and collector-base voltage (Vcb). The maximum power dissipation (Pd) is also listed in the specs. All three terminals of the transistor must be properly connected in order to use the device correctly.
The 2N4410 transistor operates in three different modes: cut-off, saturation and active. When in cut-off mode, the transistor gate is open, i.e. no current flows through the transistor. This can be experienced by connecting the collector to the emitter and applying 0V to the base terminal. The transistor is then said to be cut off and no current will flow through it. In saturation mode, the transistor gate is closed, i.e. current is flowing from the collector to the emitter. This can be seen by connecting the base to the emitter and applying 1V to the collector. The transistor is then said to be saturated, meaning current is flowing from the collector to the emitter.
In active mode, the transistor gate is partially open and some current is flowing through the transistor. This state is experienced by connecting the base to the emitter and applying a voltage in between 0V and 1V to the collector. The amount of current flowing depends on the voltage applied.
The working principle of the 2N4410 is based on the variation of the current gain. This is the ratio of the collector current (Ic) over the base current (Ib). This current gain is calculated using the formula β=Ic/Ib. The higher the current gain, the higher the power output of the transistor. This current gain is also affected by the collector voltage. Increasing the collector voltage will reduce the current gain and result in a lower power output.
The 2N4410 is a great choice for various applications due to its optimal dc and ac performance. For example, it can be used as a switch, a high-gain amplifier, an oscillator, a low-power logic device and a protection device for voltage regulation. It is also used for low frequency linear applications such as small radio circuits, switching circuits and digital logic circuits.
Overall, the 2N4410 NPN silicon transistor is an incredibly versatile device that is able to operate in a variety of applications with excellent performance. From low-power audio amplifying applications to linear circuits, the 2N4410 is an excellent choice. By understanding the working principles of this transistor and its specified ratings, it becomes easier to make the right choice for any application.
The specific data is subject to PDF, and the above content is for reference
| Part Number | Manufacturer | Price | Quantity | Description |
|---|
| 2N4403 | Central Semi... | -- | 3118 | TRANS PNP 40V 0.6A TO-92B... |
| 2N4416A-E3 | Vishay Silic... | 0.0 $ | 1000 | MOSFET N-CH 35V 5MA TO-20... |
| 2N4403RLRM | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
| 2N4401T93 | ROHM Semicon... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
| 2N4403-AP | Micro Commer... | 0.02 $ | 12000 | TRANS PNP 40V TO92Bipolar... |
| 2N4400TAR | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
| 2N4403RLG | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
| 2N4403_S00Z | 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... |
| 2N4401_J25Z | 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... |
| 2N4410 | Central Semi... | 0.0 $ | 1000 | TRANS NPN 80V 0.25A TO-92... |
| 2N4401_J61Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
| 2N4403_D11Z | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
| 2N4400TF | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
| 2N4416A-2 | Vishay Silic... | 0.0 $ | 1000 | MOSFET N-CH 35V 5MA TO-20... |
| 2N4402_J14Z | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
| 2N4401RLRPG | ON Semicondu... | -- | 1000 | TRANS NPN 40V 0.6A TO-92B... |
| 2N4401TFR | ON Semicondu... | -- | 34000 | TRANS NPN 40V 0.6A TO-92B... |
| 2N4402_D81Z | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
| 2N4402_S00Z | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
| 2N4402TA | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
| 2N4401_S00Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
| 2N4403_J18Z | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
| 2N4401-AP | Micro Commer... | -- | 38000 | TRANS NPN 40V TO92Bipolar... |
| 2N4403_D81Z | 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... |
| 2N4403RLRA | ON Semicondu... | -- | 1000 | TRANS PNP 40V 0.6A TO92Bi... |
| 2N4410_D75Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 80V 0.2A TO-92B... |
| 2N4449 | Microsemi Co... | 10.44 $ | 1000 | TRANS NPN 20V TO46Bipolar... |
| 2N4416 | Vishay Silic... | -- | 1000 | JFET N-CH 30V 0.3W TO-206... |
| 2N4401RLRA | ON Semicondu... | -- | 1000 | TRANS NPN 40V 0.6A TO92Bi... |
| 2N4401RLRM | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 40V 0.6A TO-92B... |
| 2N4410_D27Z | ON Semicondu... | 0.0 $ | 1000 | TRANS NPN 80V 0.2A TO-92B... |
| 2N4401BU | ON Semicondu... | -- | 78725 | TRANS NPN 40V 0.6A TO-92B... |
| 2N4403G | ON Semicondu... | -- | 1000 | TRANS PNP 40V 0.6A TO-92B... |
| 2N4403RLRP | ON Semicondu... | 0.0 $ | 1000 | TRANS PNP 40V 0.6A TO-92B... |
| 2N4405 | Microsemi Co... | 0.0 $ | 1000 | TRANS PNP TO-39Bipolar (B... |
| 2N4403TFR | ON Semicondu... | -- | 22000 | 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...
2N4410 Datasheet/PDF