
Allicdata Part #: | M6229-ND |
Manufacturer Part#: |
1110-560K |
Price: | $ 0.00 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Bourns Inc. |
Short Description: | FIXED IND 56UH 2.8A 69 MOHM TH |
More Detail: | 56µH Unshielded Wirewound Inductor 2.8A 69 mOhm Ma... |
DataSheet: | ![]() |
Quantity: | 1000 |
1 +: | 0.00000 |
DC Resistance (DCR): | 69 mOhm Max |
Height - Seated (Max): | 0.840" (21.34mm) |
Size / Dimension: | 0.660" Dia (16.76mm) |
Supplier Device Package: | -- |
Package / Case: | Radial |
Mounting Type: | Through Hole |
Inductance Frequency - Test: | 1kHz |
Operating Temperature: | -55°C ~ 105°C |
Ratings: | -- |
Frequency - Self Resonant: | -- |
Q @ Freq: | -- |
Series: | 1110 |
Shielding: | Unshielded |
Current - Saturation: | -- |
Current Rating: | 2.8A |
Tolerance: | ±10% |
Inductance: | 56µH |
Material - Core: | Ferrite |
Type: | Wirewound |
Part Status: | Obsolete |
Packaging: | Bulk |
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Fixed inductors, also known as inductors, are two-terminal electronic components that store energy in the form of a magnetic field when a current flows through them. The 1110-560K (commonly referred to as the 1110K) fixed inductor is one of the most commonly used inductor components for commercial, industrial, and military applications. This article will discuss the application field and working principle of the 1110K.
The 1110K inductor is typically used in the complete electronic circuits, especially in the low-frequency applications. It is an ideal choice for those projects that require electrical efficiency and reliability, such as energy saving devices, voltage regulators, DC-DC converters, and motor controllers. Its usable frequency range extends from 50K Hz to 800K Hz, and it can support a huge variety of electrical loads, from very small to large currents, while consuming less electrical energy. Furthermore, its compatible package provides space savings, allowing the circuit designers to use fewer components in a given design.
The 1110K inductor works by generating a magnetic field in a metal core when an electrical current passes through its windings. This magnetic field then induces a voltage in the windings of the inductor, which in turn can discharge energy from the inductor. The basic working principle of the 1110K inductor can be further broken down into two major parts: inductive reactance and magnetic saturation.
Inductive reactance, also referred to as the opposition to a change in current, is the characteristic of the inductor that opposes increases or decreases in the flow of electric current. When supplying a steady amount of current to the 1110K inductor, the inductance of the component will increase, causing a greater resistance to the flow of current and decreasing the effectiveness of the energy discharged from the inductor. In addition, when supplying a diminishing amount of current to the 1110K inductor, the inductance of the component will decrease, allowing greater amounts of current to flow and increasing the effectiveness of energy discharged from the inductor.
The other major general principle behind the 1110K inductor is magnetic saturation. Much like inductive reactance, magnetic saturation is the resistance to a change in the magnetic field strength within the core material of the inductor. When the intensity of the magnetic field reaches a particular level, the inductor will reach magnetic saturation, leading to an increased resistance to an increased magnetic field. Because the 1110K inductor has a higher capacity for magnetic saturation than most other types of inductors, it is an ideal component for use in applications that require a high magnetic field strength.
In conclusion, the 1110K fixed inductor is one of the most commonly used inductor components for commercial, industrial, and military applications due to its widely utilized application field and unique working principles. By incorporating inductive reactance and magnetic saturation, the 1110K can be a reliable, energy efficient, and space-saving component in many electronic circuits.
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