HKQ0603U3N2S-T Allicdata Electronics
Allicdata Part #:

HKQ0603U3N2S-T-ND

Manufacturer Part#:

HKQ0603U3N2S-T

Price: $ 0.01
Product Category:

Inductors, Coils, Chokes

Manufacturer: Taiyo Yuden
Short Description: FIXED IND 3.2NH 415MA 280 MOHM
More Detail: 3.2nH Unshielded Multilayer Inductor 415mA 280 mOh...
DataSheet: HKQ0603U3N2S-T datasheetHKQ0603U3N2S-T Datasheet/PDF
Quantity: 1000
15000 +: $ 0.00964
Stock 1000Can Ship Immediately
$ 0.01
Specifications
DC Resistance (DCR): 280 mOhm Max
Height - Seated (Max): 0.013" (0.33mm)
Size / Dimension: 0.024" L x 0.012" W (0.60mm x 0.30mm)
Supplier Device Package: 0201 (0603 Metric)
Package / Case: 0201 (0603 Metric)
Mounting Type: Surface Mount
Inductance Frequency - Test: 500MHz
Operating Temperature: -55°C ~ 125°C
Ratings: --
Frequency - Self Resonant: 8.7GHz
Q @ Freq: 14 @ 500MHz
Series: HK, Q Type
Shielding: Unshielded
Current - Saturation: --
Current Rating: 415mA
Tolerance: ±0.3nH
Inductance: 3.2nH
Material - Core: Ceramic
Type: Multilayer
Part Status: Active
Packaging: Tape & Reel (TR) 
Description

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Fixed Inductors
Fixed inductors consist of a core material, winding, and an elastomeric cover or other forms of packaging. They form an integral part of all electronic circuits, or they are grafted onto existing circuits. The inductors can be found in most electronic circuits, such as AC, DC, and pulse circuits. They provide a means of controlling current flow and voltage levels on a process level, while offering additional flexibility by providing a component that can store and induct energy. The current generated by an inductor is usually limited by a capacitor in a parallel combination.

The HKQ0603U3N2S-T is a fixed inductor manufactured by Kemet. This product specifically features a highly stable construction, with a magnetic shield to provide additional protection against EMI (ElectroMagnetic Interference). The inductor also features a low DC resistance, allowing for the desired current flow at lower power consumption, and a low ESR (Equivalent Series Resistance) that provides improved operational efficiency. Furthermore, the coil construction ensures uniform inductance across the coil and enables stable signal propagation along the inductor’s path.

The HKQ0603U3N2S-T is designed for application fields such as power management, audio mixing and amplifiers, high frequency switching, and microcontrollers, among others. These applications require a reliable inductor to help achieve high performance and low power consumption. The inductor is designed for use in a wide range of temperatures, from -55°C to +105°C. The inductor is rated at 3.0 A with a saturation current of 6.0 A.

The HKQ0603U3N2S-T works by inducing a magnetic field in the vicinity of the winding when current is passed through it, which acts to block or resist a change in the current. This property gives the HKQ0603U3N2S-T the ability to store energy temporarily, and the amount of energy stored is proportional to the value of the inductance. The value of the inductance also affects the resistance of the inductor. The resistance offered by an inductor to changes in current is given by the equation, R = 2πfL, where R is the resistance, f is the frequency, and L is the inductance.

The HKQ0603U3N2S-T is available in a range of different package sizes, with the small size of 0603 making it ideal for space constrained applications. The inductor also features high surge current and low power consumption, and the inrush current of this product is rated at 0.25 AP.

In summary, the HKQ0603U3N2S-T is a fixed inductor specially manufactured by Kemet that features a magnetic shield to prevent EMI. It is suitable for a number of applications such as power management, audio mixing and amplifiers, high frequency switching, and microcontrollers. The inductor comes in a range of package sizes and is rated at 3.0 A with a saturation current of 6.0 A. It has a low DC resistance and low ESR, making it ideal for low power consumption and high performance applications. The inductor works by inducing a magnetic field in the vicinity of a winding when current is passed through it, and the resistance of the inductor is given by the equation R = 2πfL.

The specific data is subject to PDF, and the above content is for reference

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