CDEP105NP-0R8MC-32 Allicdata Electronics
Allicdata Part #:

CDEP105NP-0R8MC-32TR-ND

Manufacturer Part#:

CDEP105NP-0R8MC-32

Price: $ 0.51
Product Category:

Inductors, Coils, Chokes

Manufacturer: Sumida America Components Inc.
Short Description: FIXED IND 800NH 11.2A 5.3 MOHM
More Detail: 800nH Shielded Wirewound Inductor 11.2A 5.3 mOhm M...
DataSheet: CDEP105NP-0R8MC-32 datasheetCDEP105NP-0R8MC-32 Datasheet/PDF
Quantity: 1000
500 +: $ 0.46494
Stock 1000Can Ship Immediately
$ 0.51
Specifications
Series: CDEP105
Packaging: Tape & Reel (TR) 
Part Status: Active
Type: Wirewound
Material - Core: Ferrite
Inductance: 800nH
Tolerance: ±20%
Current Rating: 11.2A
Current - Saturation: 25.2A
Shielding: Shielded
DC Resistance (DCR): 5.3 mOhm Max
Q @ Freq: --
Frequency - Self Resonant: --
Ratings: --
Operating Temperature: -40°C ~ 125°C
Inductance Frequency - Test: 100kHz
Mounting Type: Surface Mount
Package / Case: Nonstandard
Supplier Device Package: --
Size / Dimension: 0.394" L x 0.394" W (10.00mm x 10.00mm)
Height - Seated (Max): 0.220" (5.60mm)
Description

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Fixed inductors, such as the CDEP105NP-0R8MC-32, are a type of electrical component used to provide signal filtering, decoupling or to act as an energy storage element in an electrical circuit. The device is composed of copper windings, ceramic core and various other components as required. Its small size makes it ideal for use in small electronic circuitry and its ability to handle frequencies ranging from the low Hz up to the ultra high frequency (UHF) range makes it incredibly versatile.

The CDEP105NP-0R8MC-32 is a type of axial lead power inductor component consisting of a ferrite core with an axial lead wire. The device has a maximum inductance of 0.8 mH. Its maximum current capability is 2.7A, and its maximum DC resistance is 0.15. It has an operating temperature of up to +125°C and a maximum power dissipation of 0.6 watts. The frequency range of this inductor is from 50 kHz to 200kHz.

The device is ideal for use in applications such as DC-DC converters, voltage regulators, amplifiers, LED lighting, telecommunication and RF circuits. Its main function is to filter or decouple signals or frequencies from an electrical circuit. It also works to increase the current at low frequencies, act as an energy storage element and reduce the reactance of capacitors in an electrical circuit.

The working principle of the CDEP105NP-0R8MC-32 is rooted in the properties of an ideal inductor. An ideal inductor behaves like an open-circuited primary in the case of an alternating current. The magnetic field is produced when current passes through the inductor, and the field then induces a voltage in the inductor. The voltage is also determined by the frequency and amount of current passing through the inductor. This behavior is referred to as the voltage-current relationship of an inductor.

The fundamental equation of the voltage-current relationship for an inductor is given by: V = L di/dt, where V is the induced voltage, L is the inductance of the inductor, i is the current flowing through the inductor and t is the time. The equation states that the induced voltage is proportional to the change in current over time and is determined by the inductance of the inductor.

When the CDEP105NP-0R8MC-32 is installed in a circuit, the current passing through the device increases as the current increases and vice versa. In AC circuits, the frequency and amplitude of the current will fluctuate, which produces a varying induced voltage. This varying voltage is then able to filter, decouple and limit the current as required.

In conclusion, the CDEP105NP-0R8MC-32 fixed inductor is a versatile and powerful component that can be used for a variety of applications. It is composed of a copper winding, ceramic core and various other components and is capable of handling frequencies ranging from the low Hz up to the UHF range. The device is ideal for use in DC-DC converters, voltage regulators, amplifiers, LED lighting, telecommunication and other RF circuits. It works on the principle of the voltage-current relationship of an ideal inductor, where the induced voltage is dependent on the frequency and amount of current passing through the inductor.

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

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