Allicdata Part #: | MJF6388OS-ND |
Manufacturer Part#: |
MJF6388 |
Price: | $ 0.00 |
Product Category: | Discrete Semiconductor Products |
Manufacturer: | ON Semiconductor |
Short Description: | TRANS NPN DARL 100V 10A TO220FP |
More Detail: | Bipolar (BJT) Transistor NPN - Darlington 100V 10A... |
DataSheet: | MJF6388 Datasheet/PDF |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | -- |
Packaging: | Tube |
Part Status: | Obsolete |
Transistor Type: | NPN - Darlington |
Current - Collector (Ic) (Max): | 10A |
Voltage - Collector Emitter Breakdown (Max): | 100V |
Vce Saturation (Max) @ Ib, Ic: | 3V @ 100mA, 10A |
Current - Collector Cutoff (Max): | 10µA |
DC Current Gain (hFE) (Min) @ Ic, Vce: | 3000 @ 3A, 4V |
Power - Max: | 2W |
Frequency - Transition: | -- |
Operating Temperature: | -65°C ~ 150°C (TJ) |
Mounting Type: | Through Hole |
Package / Case: | TO-220-3 Full Pack |
Supplier Device Package: | TO-220FP |
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The MJF6388 is a single bipolar junction transistor (BJT) designed for low-power and medium-power amplifying purposes. This transistor is designed with a very shallow base region and wide base-to-emitter junction, which provides superior gain and power over other BJTs. This also allows for a current gain of up to 770. The main applications areas for the MJF6388 are small signal amplifying circuits, power amplifiers, and general-purpose analog circuits.
The main operating principles for the MJF6388 involve four core components: the base, the emitter, the collector, and the B-E junction. The base is the control point of the BJT, and the emitter and collector are the two output points in the transistor. As current into the base is increased, more current can flow between the emitter and collector. This current flow is determined by the BJT’s B-E junction, as it acts as both a resistive and capacitive element in the circuit. For a BJT, the approximate gain, or current amplification factor, is calculated using the formula Hfe = [Ic/Ib]. This gain characteristic is determined by the B-E junction.
The MJF6388 is rated for a maximum collector-emitter voltage of 160 V and an integral power dissipation of 400 mW. It is manufactured in a TO-92 package, which makes it well suited for low-power and high-efficiency applications. Another advantage of the TO-92 package is its low thermal resistance, which allows for superior heat transfer properties. Additionally, the MJF6388 exhibits good thermal stability, making it suitable for temperature-critical applications.
The MJF6388 features a high output current capability combined with a low saturation voltage. This low saturation voltage is important for applications where stability and accuracy must be maintained. The MJF6388 also has a low noise level and is resistant to reverse biasing, making it well suited for signal-processing applications. Its high output current capability also makes it suitable for power amplifying purposes.
The MJF6388 can simplify the design process by reducing the need to use multiple transistors in a design. This reduces the complexity of the design process, as well as the parts count and cost. In addition, its low thermal resistance allows it to be used in high-temperature applications without the need to use additional cooling methods. This makes the MJF6388 a useful alternative for applications that require superior performance from a single BJT.
In conclusion, the MJF6388 is a low-power and medium-power single BJT designed for amplifying purposes. Its shallow base region and wide B-E junction provide it with superior gain and power over other BJTs. It is packaged in a TO-92 package, which allows for excellent thermal transfer properties. Furthermore, it exhibits good thermal stability and a high output current capability. It also simplifies the design process by reducing the need to use multiple transistors in a design. As such, the MJF6388 is a great choice for low-power and medium-power amplifying applications.
The specific data is subject to PDF, and the above content is for reference
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