1025-86J

DC Resistance (DCR):	46 Ohm Max
Height - Seated (Max):	--
Size / Dimension:	0.095" Dia x 0.250" L (2.41mm x 6.35mm)
Supplier Device Package:	Axial
Package / Case:	Axial
Mounting Type:	Through Hole
Inductance Frequency - Test:	790kHz
Operating Temperature:	-55°C ~ 105°C
Ratings:	--
Frequency - Self Resonant:	5MHz
Q @ Freq:	30 @ 790kHz
Series:	1025
Shielding:	Unshielded
Current - Saturation:	--
Current Rating:	35mA
Tolerance:	±5%
Inductance:	560µH
Material - Core:	Ferrite
Type:	Molded
Part Status:	Active
Packaging:	Tape & Reel (TR)

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

Fixed Inductors: 1025-86J Application Field and Working Principle

An inductor is an electrical component used to store energy in its magnetic field. Much like a capacitor, they are used in a variety of applications, including the filtering of signals and the conversion of alternating current (AC) to direct current (DC). Fixed inductors are versatile components, but 1025-86J inductors have been gaining more attention over the past several years due to their unique properties and applications.

In terms of applications, 1025-86J fixed inductors are highly popular among electronics engineers. This type of inductor is best suited for applications where waveform distortion needs to be minimized. These types of inductors can also be used in radio frequency (RF) applications, and they provide very stable performance with wide temperature ranges. They are particularly useful in applications such as eliminating electromagnetic interference (EMI) and suppressing transient voltage spikes. The 1025-86J inductors are also well-suited for radio frequency interference (RFI) and signal integrity applications. They are also suitable for use in industrial automation applications, as they provide stable performance and distortion-free signals.

In terms of construction, the 1025-86J fixed inductors are made of high-temperature grade ceramics. These components are constructed with a ceramic core surrounded by a ferrite material, which is then wound with high temperature grade wire to form the final inductor. This construction ensures that the core does not overheat and increases the overall reliability of the component. The 1025-86J inductors have a typical inductance range of 7.6-17.6uH for most packages, allowing for a wide range of operating frequencies. Additionally, the 1025-86J can withstand currents up to 4.5A.

The working principle behind the 1025-86J fixed inductor is simple. The core material is able to store energy in the form of a magnetic field when a current is passed through it. This magnetic field opposes a change in the current, allowing for an increase in voltage over the inductor. This property gives the inductor a wide range of applications, from smoothing out a signal in radio frequency applications to eliminating electromagnetic interference in industrial automation systems. The 1025-86J inductor also has a self-resonance frequency of around 150MHz, allowing it to be used in high frequency circuits with minimal distortion.

Overall, the 1025-86J series of fixed inductors provides electronics engineers with an invaluable tool for minimizing waveform distortion in a wide range of applications. The components are highly reliable, have wide temperature ranges, and can be used in both radio frequency and signal integrity applications. The components are also suitable for industrial automation, as they act to eliminate EMI and stifle transient voltage spikes. Finally, their self-resonance frequency allows for high accuracy and clarity in high frequency circuits. As such, the 1025-86J series of fixed inductors is a valuable addition to the arsenal of any electronics engineer.

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

Part Number	Manufacturer	Price	Quantity	Description