| Allicdata Part #: | B82432C1823J000-ND |
| Manufacturer Part#: |
B82432C1823J000 |
| Price: | $ 0.27 |
| Product Category: | Inductors, Coils, Chokes |
| Manufacturer: | EPCOS (TDK) |
| Short Description: | FIXED IND 82UH 175MA 3.2 OHM SMD |
| More Detail: | 82µH Unshielded Wirewound Inductor 175mA 3.2 Ohm M... |
| DataSheet: | B82432C1823J000 Datasheet/PDF |
| Quantity: | 1000 |
| 5000 +: | $ 0.24409 |
| DC Resistance (DCR): | 3.2 Ohm Max |
| Height - Seated (Max): | 0.134" (3.40mm) |
| Size / Dimension: | 0.177" L x 0.126" W (4.50mm x 3.20mm) |
| Supplier Device Package: | 1812 (4532 Metric) |
| Package / Case: | 2-SMD, J-Lead |
| Mounting Type: | Surface Mount |
| Inductance Frequency - Test: | 100kHz |
| Operating Temperature: | -55°C ~ 125°C |
| Ratings: | AEC-Q200 |
| Frequency - Self Resonant: | 9MHz |
| Q @ Freq: | 30 @ 2.52MHz |
| Series: | SIMID |
| Shielding: | Unshielded |
| Current - Saturation: | -- |
| Current Rating: | 175mA |
| Tolerance: | ±5% |
| Inductance: | 82µH |
| Material - Core: | Ferrite |
| Type: | Wirewound |
| Part Status: | Active |
| Packaging: | Tape & Reel (TR) |
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Fixed Inductors
The B82432C1823J000 is a fixed inductor, and it is used in a variety of applications. An inductor is a passive electronic component that stores energy in the form of a magnetic field when a current is applied. The B82432C1823J000 is suitable for high frequency applications as it is capable of storing energy up to 500MHz. As well as frequency limitations, the B82432C1823J000 has current handling capabilities of up to 4A.
Application Fields
The B82432C1823J000 is a versatile component and is utilised in a wide variety of applications. It is mainly used in filters, voltage-controlled oscillators (VCOs), frequency dividers, switching power supplies and in shielding low electromagnetic interference signals. It has also been utilised in wireless communication systems in various products, making the B82432C1823J000 an integral part of the industry.
Working Principle
The inductor works on Faraday’s law of induction, which states that when a conductor is exposed to an electric field, a current is induced. When a current passes through a core of the inductor, a magnetic field is created, which in turn, induces a voltage proportional to the rate of change of the current flow. This means that the induced voltage is proportional to the rate of change of the current flow. The B82432C1823J000 works in this very way, as an inductor it will produce a magnetic field when current passes through its core and so if the current is decreasing, the induced voltage will be negative.
Furthermore, the B82432C1823J000 has a nonlinear core shape, which allows for an increased capability in terms of frequency response and current handling capability. This feature makes the B82432C1823J000 a popular choice in high frequency applications.
The specific data is subject to PDF, and the above content is for reference
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B82432C1823J000 Datasheet/PDF