5400-106G

DC Resistance (DCR):	1.53 Ohm Max
Height - Seated (Max):	0.730" (18.54mm)
Size / Dimension:	1.300" Dia (33.02mm)
Supplier Device Package:	--
Package / Case:	Radial
Mounting Type:	Through Hole
Inductance Frequency - Test:	1kHz
Operating Temperature:	-55°C ~ 125°C
Ratings:	--
Frequency - Self Resonant:	269kHz
Q @ Freq:	--
Series:	5400
Shielding:	Unshielded
Current - Saturation:	204mA
Current Rating:	204mA
Tolerance:	±2%
Inductance:	10mH
Material - Core:	Iron Powder
Type:	--
Part Status:	Active
Packaging:	Bulk

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Fixed inductors, such as 5400-106G, are an essential component of modern electronics. These components have become indispensable in a wide variety of circuits and applications. In this article, we will discuss the application field and working principle of fixed inductors and the 5400-106G in particular.Fixed inductors are wound electrical components used mainly for storing energy in the form of a magnetic field. They are ubiquitous in electronic circuits; a basic electronic device such as a mobile phone circuit board contains dozens of inductors. They are usually composed of a conducting wire enclosing an air core. They are also available as ferrite core and crystal core in different configurations.In addition to their electrical function in storage, fixed inductors provide high-frequency filtering, impedance transformation, and act as RF-shields. They are also used to couple information signals between two different network components. Furthermore, they are useful for damping oscillations and delay signals.The 5400-106G fixed inductor is a radial-leaded component and stands out from other inductors in its stability and robustness. It is designed to be used in critical applications such as automotive systems, power supplies, and medical equipment. Due to its operating frequency range of 1MHz – 200MHz, the device can handle fast and high-capacity transmitted data. The 5400-106G has an inductance of 10μH. Its maximum DC current is rated at 106 A and its maximum DC resistance is 0.008 Ω. The temperature coefficient of resistance is 0.9% per K, and the saturation current is 37.2 A. Additionally, the 5400-106G has a high tolerance of ±5%. The working principle of the 5400-106G inductor can be explained using Faraday\'s law of induction. In essence, when a wire carrying an electric current is encased in a magnetic field, a voltage is induced in the wire due to the movement of electrons. This voltage is known as a back-EMF, and it is proportional to the rate of change of the magnetic field. In the case of the 5400-106, the rate of change of the magnetic field is proportional to the current in the wire – when the current is increased, the magnetic field increases proportionally, which in turn induces a voltage. Thus, the 5400-106G inductor works as a converter of electric energy into magnetic energy, and vice versa. To conclude, fixed inductors are a basic but indispensable part of electronics. The 5400-106G inductor is a prime example of this, and offers robustness, stability, and high frequency filtering capability. Its operation is based on Faraday\'s law of induction. It is suitable for a range of applications and can be used in fast, high-intensive transmitted data systems.

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