2N4857 Allicdata Electronics
Allicdata Part #:

2N4857-ND

Manufacturer Part#:

2N4857

Price: $ 0.00
Product Category:

Discrete Semiconductor Products

Manufacturer: Microsemi Corporation
Short Description: N CHANNEL JFET
More Detail: JFET N-Channel 40V 360mW Through Hole TO-18
DataSheet: 2N4857 datasheet2N4857 Datasheet/PDF
Quantity: 1000
Stock 1000Can Ship Immediately
Specifications
Series: Military, MIL-PRF-19500/385
Packaging: Bulk 
Part Status: Active
FET Type: N-Channel
Voltage - Breakdown (V(BR)GSS): 40V
Drain to Source Voltage (Vdss): 40V
Current - Drain (Idss) @ Vds (Vgs=0): 100mA @ 15V
Voltage - Cutoff (VGS off) @ Id: 6V @ 500pA
Input Capacitance (Ciss) (Max) @ Vds: 18pF @ 10V
Resistance - RDS(On): 40 Ohms
Power - Max: 360mW
Operating Temperature: -65°C ~ 200°C (TJ)
Mounting Type: Through Hole
Package / Case: TO-206AA, TO-18-3 Metal Can
Supplier Device Package: TO-18
Description

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

Transistors are one of the most important components in our electronics industry. As one of the most widely used transistors, the junction gate field-effect transistors (JFETs) are widely used in our everyday electronics. The JFETs are widely used because of their excellent performance and reliability. The 2N4857 is one of the most widely used JFETs. In this article, we will discuss the application field and working principle of the 2N4857.

The 2N4857 are designed as low-noise, high-gain general-purpose JFETs and can be used in many different applications. They can be used as amplifiers, oscillators, active filters and so on. The 2N4857 can also be used for low-level and high-power switching. They have the capability of switching both AC and DC signals. They are also ideal for high gain, low-noise audio applications. The 2N4857 is also suitable for low-noise cathode-follower applications.

The 2N4857 has a P-Channel construction, which means that when there is positive bias applied to the gate it creates a depletion region in the channel between drain and source, making the channel more resistant to current flow. The higher the voltage applied to the gate, the more depletion region created, and the more blocking effect that the JFET will have. The higher the gate voltage, the lower the current flow will be between drain and source. The 2N4857 can operate with a wide range of supply voltages and is capable of handling a large amount of current at high frequencies.

The working principle of the 2N4857 is quite simple. It is basically a solid-state device that is composed of a single, p-type semiconductor material. The material is composed of atoms that have three different states: Electron, Hole and Neutral.The electrons are most mobile in the electron state, and they can move in the semiconductor material freely. The hole state is then created when the electrons are moved across, leaving a hole in the semiconductor material that has a positive charge. The neutral state is then created when the holes and electrons come together again.

The operation of the 2N4857 is based on the interaction between the gate voltage and the voltage applied to the source and drain. When the voltage is applied to the gate, it generates a depletion region in the channel between the drain and the source. This reduces the flow of current between the drain and the source. The higher the voltage to the gate, the more depletion region is generated, and the more blocking effect the JFET will have.

In conclusion, the 2N4857 is one of the most popular JFETs due to its excellent performance and versatility. The 2N4857 has a P-Channel construction and is capable of handling large currents at high frequencies. The 2N4857 can be used in many different applications, such as amplifiers, oscillators, and active filters. The working principle of the 2N4857 is based on the interaction between the gate voltage and the voltage applied to the source and drain. This creates a depletion region in the channel between the drain and the source, reducing the flow of current. The higher the gate voltage, the more blocking effect the JFET will have.

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

Related Products
Search Part number : "2N48" Included word is 40
Part Number Manufacturer Price Quantity Description
2N4854UTX TT Electroni... 18.73 $ 1000 TRANS NPN/PNP 40V 0.6A 6C...
2N4857UB Microsemi Co... 55.79 $ 1000 N CHANNEL JFETJFET
2N4857JTXV02 Vishay Silic... 0.0 $ 1000 JFET N-CH 40V 360MA TO-18...
2N4857JTXL02 Vishay Silic... 0.0 $ 1000 JFET N-CH 40V 360MA TO-18...
2N4860JTXL02 Vishay Silic... 0.0 $ 1000 JFET N-CH 30V TO-206JFET ...
2N4858JTXV02 Vishay Silic... 0.0 $ 1000 JFET N-CH 40V 80MA TO-18J...
2N4856JTXL02 Vishay Silic... 0.0 $ 1000 MOSFET N-CH 40V 50MA TO-1...
2N4858A Central Semi... -- 870 JFET N-CH 40V 0.36W TO-18...
2N4856 Microsemi Co... -- 1000 N CHANNEL JFETJFET N-Chan...
2N4895 Central Semi... 8.88 $ 408 TRANS NPN 60V TO39Bipolar...
2N4859JTX02 Vishay Silic... 0.0 $ 1000 JFET N-CH 30V 360MW TO-18...
2N4860UB Microsemi Co... 55.79 $ 1000 N CHANNEL JFETJFET
2N4854 Central Semi... 0.0 $ 1000 TRANSISTOR DUAL TO78Bipol...
2N4898 Microsemi Co... 24.45 $ 1000 NPN SILICON TRANSISTORBip...
2N4859JTXV02 Vishay Silic... 0.0 $ 1000 JFET N-CH 30V 360MW TO-18...
2N4861JTX02 Vishay Silic... 0.0 $ 1000 JFET N-CH 30V TO-206JFET ...
2N4871 Central Semi... -- 1165 THROUGH-HOLE TRANSISTOR-S...
2N4870 Central Semi... 0.81 $ 1000 THROUGH-HOLE TRANSISTOR-S...
2N4858 Microsemi Co... -- 1000 N CHANNEL JFETJFET N-Chan...
2N4856JTX02 Vishay Silic... 0.0 $ 1000 MOSFET N-CH 40V 50MA TO-1...
2N4857 Microsemi Co... -- 1000 N CHANNEL JFETJFET N-Chan...
2N4858JTX02 Vishay Silic... 0.0 $ 1000 JFET N-CH 40V 80MA TO-18J...
2N4899 Microsemi Co... 24.45 $ 1000 NPN SILICON TRANSISTORBip...
2N4859 Microsemi Co... 39.43 $ 1000 N CHANNEL JFETJFET N-Chan...
2N4861JTXV02 Vishay Silic... 0.0 $ 1000 JFET N-CH 30V TO-206JFET ...
2N4865 Microsemi Co... 7.68 $ 1000 NPN SILICON TRANSISTORBip...
2N4859A Central Semi... 0.0 $ 1000 JFET N-CH 30V 50MA 360MW ...
2N4860JTXV02 Vishay Silic... 0.0 $ 1000 JFET N-CH 30V TO-206JFET ...
2N4860 Microsemi Co... 39.43 $ 1000 N CHANNEL JFETJFET N-Chan...
2N4859JTXL02 Vishay Silic... 0.0 $ 1000 JFET N-CH 30V 360MW TO-18...
2N4859UB Microsemi Co... 55.79 $ 1000 N CHANNEL JFETJFET
2N4859JAN02 Vishay Silic... 0.0 $ 1000 JFET N-CH 30V 360MW TO-18...
2N4861JAN02 Vishay Silic... 0.0 $ 1000 JFET N-CH 30V TO-206JFET ...
2N4854U TT Electroni... 22.89 $ 50 TRANS NPN/PNP 40V 0.6A 6C...
2N4858JAN02 Vishay Silic... 0.0 $ 1000 JFET N-CH 40V 80MA TO-18J...
2N4858JTXL02 Vishay Silic... 0.0 $ 1000 JFET N-CH 40V 80MA TO-18J...
2N4856UB Microsemi Co... 55.79 $ 1000 N CHANNEL JFETJFET
2N4857JAN02 Vishay Silic... 0.0 $ 1000 JFET N-CH 40V 360MA TO-18...
2N4856JAN02 Vishay Silic... 0.0 $ 1000 MOSFET N-CH 40V 50MA TO-1...
2N4860JAN02 Vishay Silic... 0.0 $ 1000 JFET N-CH 30V TO-206JFET ...
Latest Products
J3A080YXS/T0BY4AG0

TRANSISTOR JFET 8PLLCCTRANSISTOR JFET 8P...

J3A080YXS/T0BY4AG0 Allicdata Electronics
J3A040YXS/T0BY4571

TRANSISTOR JFET 8PLLCCTRANSISTOR JFET 8P...

J3A040YXS/T0BY4571 Allicdata Electronics
J3A012YXS/T0BY4551

TRANSISTOR JFET 8PLLCCTRANSISTOR JFET 8P...

J3A012YXS/T0BY4551 Allicdata Electronics
J2A080GX0/T0BG295,

TRANSISTOR JFET 8PLLCCTRANSISTOR JFET 8P...

J2A080GX0/T0BG295, Allicdata Electronics
J2A040YXS/T0BY424,

TRANSISTOR JFET 8PLLCCTRANSISTOR JFET 8P...

J2A040YXS/T0BY424, Allicdata Electronics
J2A020YXS/T0BY425,

TRANSISTOR JFET 8PLLCCTRANSISTOR JFET 8P...

J2A020YXS/T0BY425, Allicdata Electronics