P1169.823NLT

Q @ Freq:	--
Height - Seated (Max):	0.177" (4.50mm)
Size / Dimension:	0.482" L x 0.482" W (12.24mm x 12.24mm)
Supplier Device Package:	--
Package / Case:	Nonstandard
Mounting Type:	Surface Mount
Features:	--
Inductance Frequency - Test:	100kHz
Operating Temperature:	-40°C ~ 130°C
Ratings:	--
Frequency - Self Resonant:	6MHz
Series:	P1169NL
DC Resistance (DCR):	232 mOhm Max
Shielding:	Shielded
Current - Saturation:	1.4A
Current Rating:	1.4A
Tolerance:	±20%
Inductance:	82µH
Material - Core:	--
Type:	Wirewound
Part Status:	Active
Packaging:	Tape & Reel (TR)

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P1169.823NLT Fixed InductorsInductors are electronic components designed to store energy in the form of an electro-magnetic field. The P1169.823NLT is a fixed inductor, meaning that it is made with a solid core whose parameters cannot be changed. While it may look like a simple resistor, there are many ways that an inductor can be used in electronic circuits. The P1169.823NLT fixed inductor has many applications in various circuits. It can be used to filter high-frequency signals, act as an impedance-matching network, act as an input filter for power supplies, and even help reduce electrical noise. These versatile components can also be used to measure and control current in a circuit as well as in adjustable power supplies.The working principle of the P1169.823NLT is that of any other inductor. It reacts to any changes in the current passing through it by inducting an opposing voltage. This opposing voltage is proportional to the rate of change of the current and is referred to as self-inductance.The P1169.823NLT is made up of two parts: a wire coil and a core. The wire coil is made up of multiple turns of a conductor, such as copper or aluminum, while the core is a ferromagnetic material such as iron. Together, these two components form an inductor. The core creates the magnetic field that stores the energy and is the key to understanding how the inductor works. When current is applied to the wire coil, a magnetic field is generated in the core. This field is proportional to the current passing through the coil and it resists any changes in current, resulting in an inductance. The inductance of an inductor is measured in Henries. In the case of the P1169.823NLT, the inductance is 2.6 uH. This is the range of inductance in which the component operates best. The inductance increases as the number of turns in the wire coil increases and decreases as the cross-sectional area of the core decreases.In addition to the inductance, the P1169.823NLT also has a self-resonant frequency. This is the frequency at which the inductance of the inductor is at a maximum. For the P1169.823NLT, the self-resonant frequency is approximately 5.9 MHz.The P1169.823NLT also has an out-of-plane resistance. This is the resistance in the magnetic field created by the inductor. The out-of-plane resistance of the P1169.823NLT is approximately 20 mOhms.The P1169.823NLT is a versatile and reliable component that can be used in applications such as filtering, impedance-matching networks, noise reduction, and more. It is made up of a wire coil and a core and operates on the principle of generating a magnetic field proportional to the current passing through it. The inductance of the P1169.823NLT is 2.6 uH, and it has a self-resonant frequency of approximately 5.9 MHz and an out-of-plane resistance of 20 mOhms.

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