Allicdata Part #: | PN4861-ND |
Manufacturer Part#: |
PN4861 |
Price: | $ 0.00 |
Product Category: | Discrete Semiconductor Products |
Manufacturer: | ON Semiconductor |
Short Description: | JFET N-CH 30V 625MW TO92 |
More Detail: | JFET N-Channel 30V 625mW Through Hole TO-92-3 |
DataSheet: | PN4861 Datasheet/PDF |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | -- |
Packaging: | Bulk |
Part Status: | Obsolete |
FET Type: | N-Channel |
Voltage - Breakdown (V(BR)GSS): | 30V |
Current - Drain (Idss) @ Vds (Vgs=0): | 8mA @ 15V |
Voltage - Cutoff (VGS off) @ Id: | 800mV @ 0.5nA |
Input Capacitance (Ciss) (Max) @ Vds: | 18pF @ 10V |
Resistance - RDS(On): | 60 Ohms |
Power - Max: | 625mW |
Operating Temperature: | -55°C ~ 150°C (TJ) |
Mounting Type: | Through Hole |
Package / Case: | TO-226-3, TO-92-3 (TO-226AA) |
Supplier Device Package: | TO-92-3 |
Base Part Number: | 2N4861 |
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
A PN4861 is an n-channel junction gate field effect transistor (JFET). JFETs are typically used in amplifier and digital logic circuits and are constructed from materials such as silicon or germanium. A PN4861 is one of the more common type of JFET and has a much higher voltage drainage and current handling capabilities than other types. As such, it is often used for applications requiring higher power output and better heat dissipation.
The PN4861\'s fundamental working principle is essentially the same as other JFETs. It is a three terminal device comprising of the source, gate, and drain. It is controlled by an electric field that exists between the gate and the source, essentially forming a gate or diode between them. This gate or diode essentially creates an inversion layer which maintains the depletion region between the two electrodes. The amount of current between the two electrodes is proportional to the amount of voltage applied to the gate.
The PN4861 is mainly used in various switching and amplifying circuits. It is an ideal choice for applications that require high input impedance, low noise and low power dissipation. The PN4861 is also commonly used in voltage-controlled oscillators (VCO), filters, low-noise amplifiers (LNA), radio-frequency amplifiers (RF), audio amplifiers, and many other applications. In addition, its low-level detection and high-level tuning applications make it a valuable component for many integrated circuits.
The PN4861 is an ideal device for applications requiring low power dissipation and high input impedance. It is also used in applications that require controlled gain, as the amount of current between the two electrodes is directly proportional to the voltage applied to the gate. The ability to modulate the gain of the PN4861 makes it a highly versatile and efficient device. In addition, its low-noise operation and high-frequency response make it an ideal choice for applications such as audio amplifiers, VCOs, and RF amplifiers.
In conclusion, the PN4861 is a highly versatile and efficient n-channel JFET with a wide array of applications. Its metal oxide semiconductor gate structure provides high gain and low noise operation, making it an ideal choice for many circuits. Its low power dissipation and controlled gain make it an ideal choice for applications such as low-noise amplifiers, voltage-controlled oscillators, filters, and radio-frequency amplifiers. Therefore, the PN4861 is an invaluable device for those applications that require high input impedance, low power dissipation, and high performance.
The specific data is subject to PDF, and the above content is for reference
TRANSISTOR JFET 8PLLCCTRANSISTOR JFET 8P...
TRANSISTOR JFET 8PLLCCTRANSISTOR JFET 8P...
TRANSISTOR JFET 8PLLCCTRANSISTOR JFET 8P...
TRANSISTOR JFET 8PLLCCTRANSISTOR JFET 8P...
TRANSISTOR JFET 8PLLCCTRANSISTOR JFET 8P...
TRANSISTOR JFET 8PLLCCTRANSISTOR JFET 8P...