0819-76H

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Fixed Inductors

Inductors are electronic components that store energy in a magnetic field when current is applied to them. Fixed inductors, also referred to as inductors or chokes, are among the most commonly used components in circuit designs. The 0819-76H fixed inductor is an example of a popular and widely used fixed inductor.

The 0819-76H fixed inductor is a non-polarized, axial-leaded inductor that features a high self-resonance frequency and low DC resistance. It is designed with a ceramic core and wrapped in an enameled wire for enhanced stability and reliability. The 0819-76H is particularly suitable for high frequency circuits due to its high self-resonance frequency of 1MHz. This inductor is available in a wide range of sizes, having a maximum inductance value of 1μH.

The 0819-76H fixed inductor is mainly used in resonant circuits and in RF circuits, as it has a high self-resonance frequency and low DC resistance. It is also commonly used in DC/DC converters, high power amplifiers, and switching power supplies. In addition, this fixed inductor is also used for high-power inductive heating applications, such as heating elements for diathermy machines.

The working principle of the 0819-76H fixed inductor is based on Faraday’s Law, which states that a changing magnetic field induces a voltage that is proportional to the rate of change of current. In this case, when a current is applied to the inductor, a magnetic field is created around it. This field then induces a voltage across the inductor. The amount of voltage induced depends on the rate of the changing magnetic field as well as the inductance of the inductor.

The 0819-76H fixed inductor is a reliable and robust component that is suitable for a wide range of applications. It is designed for high frequency circuits and is suitable for use in DC/DC converters, RF circuits, high power amplifiers, and high power inductive heating applications. The working principle of the 0819-76H fixed inductor is based on Faraday’s Law, which states that a changing magnetic field induces a voltage that is proportional to the rate of change of current.

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