S1008-121J

Series:	S1008
Packaging:	Tape & Reel (TR)
Part Status:	Active
Type:	--
Material - Core:	Ferrite
Inductance:	120nH
Tolerance:	±5%
Current Rating:	1.06A
Current - Saturation:	--
Shielding:	Shielded
DC Resistance (DCR):	100 mOhm Max
Q @ Freq:	40 @ 25MHz
Frequency - Self Resonant:	368MHz
Ratings:	--
Operating Temperature:	-55°C ~ 125°C
Inductance Frequency - Test:	25MHz
Mounting Type:	Surface Mount
Package / Case:	1008 (2520 Metric)
Supplier Device Package:	1008 (2520 Metric)
Size / Dimension:	0.115" L x 0.105" W (2.92mm x 2.66mm)
Height - Seated (Max):	0.095" (2.41mm)

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Fixed Inductors

Fixed inductors refer to the use of magnetic cores and coils as integral components to convert electrical energy and reactance components. Fixed inductors are passive components that store energy in a magnetic field when an electric current is applied. They are composed of an iron core, a coil, and two electrodes, and can be used as an inductor or a transformer for power.Fixed inductors are widely used in many electronic products and circuits, such as for voltage, current, inductance, frequency transformation, tuning, filtering, and current clamping. They have a wide range of applications from power to audio and television. The S1008-121J fixed inductor is a general purpose component designed for use in radio frequency (RF) and wireless communication applications, such as cellular phones, pagers, and TVs. The S1008-121J is a low-loss inductor with high Q-factors that make it suitable for use in several different applications. The S1008-121J is a medium-range frequency-dependent inductor, with an inductance value ranging from around 3.1 to 22.3 nanohenrys. It has a high Q-factor of 900 at 1kHz and an operating temperature range of -40°C to +105°C. The inductor has a current capacity of up to 110mA, and is enclosed in a 5.1 x 5.0 x 3.2mm package. The working principle of the S1008-121J fixed inductor is based on Faraday’s Law of Induction. According to this law, when the current flowing through a conducting coil changes, a voltage is induced in the coil. This voltage is determined by the rate of change of current and the number of turns in the coil. When a current flows in the S1008-121J inductor, the coils form a magnetic field. The flux generated by the current of the coil induces a voltage on the coil. This voltage is dependent upon the amount of current flowing through the coil as well as the number of turns in the coil. To achieve the desired inductance, more turns are wrapped around the core. The exact relationship between the amount of inductance produced and the number of turns depends on several factors, including the size and shape of the core, the type of wire used for the coil, and the orientation of the core and coil. The ability of the S1008-121J inductor to efficiently generate magnetic fields makes it suitable for many applications, including voltage, current, and frequency transformation. In conclusion, the S1008-121J fixed inductor is a versatile component designed for use in many electronic circuits and applications. The component can be used for both voltage and current control, as well as frequency transformation. It has a high Q-factor of 900 at 1kHz and a wide operating temperature range from -40°C to +105°C. By taking advantage of Faraday’s Law of Induction, the S1008-121J can be used for many different purposes.

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