IHLP1616BZERR47M0H

Q @ Freq:	--
Height - Seated (Max):	0.079" (2.00mm)
Size / Dimension:	0.160" L x 0.160" W (4.06mm x 4.06mm)
Supplier Device Package:	--
Package / Case:	Nonstandard, 2 Lead
Mounting Type:	Surface Mount
Features:	--
Inductance Frequency - Test:	100kHz
Operating Temperature:	-55°C ~ 125°C
Ratings:	--
Frequency - Self Resonant:	145MHz
Series:	IHLP-1616BZ-0H
DC Resistance (DCR):	14.1 mOhm Max
Shielding:	Shielded
Current - Saturation:	13.1A
Current Rating:	8.5A
Tolerance:	±20%
Inductance:	470nH
Material - Core:	Ferrite
Type:	--
Part Status:	Active
Packaging:	Tape & Reel (TR)

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Fixed Inductors

Usually, a fixed inductor is composed of a coil of wire that is wrapped around a core, and the circuit containing it acts as an electric magnetic pathway. In this regard, the IHLP1616BZERR47M0H with the frequency range of 10 – 500 kHz, featuring the IHLP package, is used for wide range of applications.

IHLP1616BZERR47M0H Application Field

The IHLP1616BZERR47M0H is a fixed inductor mainly used in AC/DC power applications, hand-held equipment, telecommunications products – such as radios, LPTVs, cordless phones, etc., medical devices, automotive electronics, energy metering and other consumer electronics. Widely accepted in all electronic applications, this component is typically used as a storage element for the energy that is coming temporarily from a source of power. In particular, the IHLP1616BZERR47M0H enables:

• Efficiency and performance in energy conversion systems in DC/DC applications.
• Filtering of electric circuit signals.
• Reduction of the circuit’s time response.
• Elimination of hum and signal alterations.
• Using in resonant circuits.

IHLP1616BZERR47M0H Working Principle

In electrical engineering, an inductor is a passive electrical element bearing the physical dimension of inductance (L) which symbolizes a conductor composed of two terminals on its ends. Consequently, when the current or voltage applied to one terminal of the component changes, the other terminal will provide an opposing force to maintain the value of the inductance. The phenomenon of this effect is described by Faraday’s law of induction. It states that the induced voltage in the inductor’s terminals is directly proportional to the rate of change of the current applied to the inductor: E = -di/dtThis means that, in the IHLP1616BZERR47M0H, when the current or voltage applied to one terminal changes, an opposing force is provided to maintain the inductance value and avoid unwanted fluctuations in the circuits. There are several methods for inducing a current into an inductor, the most common being electromagnetic induction and the action of an alternating voltage. In electromagnetic induction, changes in the magnetic field around a coil or wound inductor generate an opposing voltage to maintain a constant inductance. In the case of the IHLP1616BZERR47M0H, the alternating voltage is applied to the inductor’s terminals, inducing an opposing voltage to the current. This generates an alternating magnetic field that passes through the coil of the inductor, preventing it from building up an excessive amount of current.Finally, it can be said that the IHLP1616BZERR47M0H is an effective fixed inductor for a wide range of applications. Relying on Faraday’s law of induction, it is able to prevent the build-up of excessive current in electronic circuits, allowing for efficiency and performance in the energy conversion of DC/DC applications, filtering of electric signals, reducing the circuit’s time response, and eliminate any hum and signal alterations.

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