PC9FJ4R7K Allicdata Electronics
Allicdata Part #:

PC9FJ4R7K-ND

Manufacturer Part#:

PC9FJ4R7K

Price: $ 0.00
Product Category:

Inductors, Coils, Chokes

Manufacturer: Vishay Dale
Short Description: PC 4.7 10% F09
More Detail: 4.7µH Shielded Molded Inductor 985mA 245 mOhm Max ...
DataSheet: PC9FJ4R7K datasheetPC9FJ4R7K Datasheet/PDF
Quantity: 1000
1 +: 0.00000
Stock 1000Can Ship Immediately
$ 0
Specifications
Q @ Freq: 95 @ 7.9MHz
Height - Seated (Max): 0.270" (6.86mm)
Size / Dimension: 0.265" Dia (6.73mm)
Supplier Device Package: --
Package / Case: Radial
Mounting Type: Through Hole
Features: --
Inductance Frequency - Test: 7.9MHz
Operating Temperature: -55°C ~ 125°C
Ratings: --
Frequency - Self Resonant: 79MHz
Series: PC
DC Resistance (DCR): 245 mOhm Max
Shielding: Shielded
Current - Saturation: 985mA
Current Rating: 985mA
Tolerance: ±10%
Inductance: 4.7µH
Material - Core: --
Type: Molded
Part Status: Obsolete
Packaging: --
Description

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Fixed inductors are essential components in electronic equipment. From simple electromechanical toys to sophisticated digital devices, inductors play a significant role. PC9FJ4R7K is a kind of fixed inductor, which is widely used in various circuit designs. Here we will discuss its application field and working principle.

The PC9FJ4R7K fixed inductor has a variety of applications in various circuits. It can be used in various types of power supply circuits, such as buck-boost converters, DC-DC converters, PFC (power factor correction) circuits and so on. In automotive applications, it can be used in alternator circuits, power steering systems and dynamic braking systems. It can also be found in radiofrequency and communication circuits, audio circuits, smartphone antenna circuits, etc. Accordingly, PC9FJ4R7K is appropriate for broad application fields.

The basic principle of a fixed inductor is that it stores energy in magnetic fields when current flows through it. The current in an inductor is commonly described in terms of a changing magnetic field. When an electric current passes through the inductor, a strong magnetic field is generated. The magnetic field strength is proportional to the current through the inductor, and it induces a voltage across the inductor’s terminals. This induced voltage is often referred to as back emf and acts as an instantaneous voltage source. This back emf opposes the input voltage in an inductor circuit, resulting in an exponential decrease in current flow through the inductor.

The PC9FJ4R7K fixed inductor is usually constructed from a conductive material, such as copper wire. The conductor is usually wound into a coil shape, and the coil can be air-core or ferrite-cored. An air-core coil does not have a ferromagnetic material, whereas a ferrite-cored coil has a ferromagnetic material. This ferromagnetic material can increase the inductance of the inductor, allowing it to store more energy in the magnetic field.

By manipulating the number of turns, the length, and the cross-sectional area of the conductor, the inductance of the PC9FJ4R7K fixed inductor can be adjusted to meet different application requirements. Additionally, some PC9FJ4R7K inductors also have variable inductance, which can be controlled to add more flexibility to the circuit, allowing the current to adapt to different frequencies.

Aside from inductance, other key parameters of the PC9FJ4R7K fixed inductor to consider include its maximum current rating, maximum DC resistance, self-resonant frequency, leakage inductance, and saturation current. These factors have a significant impact on the performance of the inductor in different application fields.

In conclusion, the PC9FJ4R7K is a fixed inductor with a variety of applications. By understanding its application field and working principle, designers can choose the optimal inductor for specific circuit designs and ensure the best performance of the circuit.

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

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