
Allicdata Part #: | 28A2026-0A0-ND |
Manufacturer Part#: |
28A2026-0A0 |
Price: | $ 0.43 |
Product Category: | Filters |
Manufacturer: | Laird-Signal Integrity Products |
Short Description: | FERRITE CORE HINGED |
More Detail: | Hinged (Snap On) Ferrite Core |
DataSheet: | ![]() |
Quantity: | 1000 |
1200 +: | $ 0.39151 |
Series: | 28 |
Part Status: | Active |
Type: | Round |
Design: | Hinged (Snap On) |
Impedance @ Frequency: | -- |
Material: | 28 |
Inner Dimension: | -- |
Outer Dimension: | -- |
Ratings: | -- |
Mounting Type: | -- |
Length: | -- |
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Ferrite Cores, commonly used in cables and wiring, are used to reduce the amount of radio frequency interference (RFI) present in the signals they are designed to carry. Ferrite Cores, such as the 28A2026-0A0, utilize a variety of electromagnetic characteristics to help reduce and manage the amount of RFI that is present in the signal.
Ferrite Cores come in many shapes and sizes, ranging from small bead-like cores to large doughnut-shaped cores. One of the most common types, the 28A2026-0A0, is a bead-type ferrite core made of a special type of material that is designed to absorb and dissipate RFI. The 28A2026-0A0 also has a specific resistance rating that is used to measure the amount of RFI to be shielded.
The main purpose of a ferrite core is to provide shielding or shielding effect. The shielding effect is a reduction in electrical noise that can affect the signal as well as potentially interfere with other electronic devices in the vicinity. The 28A2026-0A0 is designed to provide this shielding effect against a wide range of RFI frequencies.
There are two main principles that are used in ferrite core design to achieve the desired shielding effect. The first is called the inductive effect, which is achieved by manipulating the electromagnetic properties of the ferrite material. The second principle used is called the magnetic effect, which is a result of the ferrite\'s ability to create a strong magnetic field around the core.
The inductive effect works by taking advantage of the magnetic properties of the ferrite material and manipulating the way that the electrons move around the core. The ferrite material is used to create opposing electrical fields that interact with the electrons as they move around the core. This causes them to be forced in a certain direction, which creates a type of shielding effect.
The magnetic effect works by creating a magnetic field around the ferrite core. This magnetic field not only blocks out the radio frequency interference, but also affects the amount of current that can be passed through the core. As the current is blocked, the overall noise level of the signal is also reduced.
The amount of shielding provided by a ferrite core will depend upon the type of material used and the size of the core itself. Different materials will provide different levels of shielding effect, so it is important to use the right one for the specific application. It is also important to choose the right size of core, as too small a core can cause excessive inductive losses.
Ferrite Cores, such as the 28A2026-0A0, are an important part of the modern electronic system. They provide effective shielding against various types of RFI without having a large impact on signal integrity. With the right application of ferrite cores, it is possible to reduce the amount of RFI present in signals, thus ensuring that the signal remains reliable and interference-free.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
28A2738-0A0 | Laird-Signal... | 1.11 $ | 5417 | FERRITE CORE 233 OHM HING... |
28A2024-0A0 | Laird-Signal... | 1.99 $ | 1000 | FERRITE CORE 280 OHM HING... |
28A2432-0A2 | Laird-Signal... | 1.31 $ | 16396 | FERRITE CORE 160 OHM HING... |
28A2736-0A2 | Laird-Signal... | 0.85 $ | 57801 | FERRITE CORE 220 OHM HING... |
DP241-5-28A26 | Pulse Electr... | 0.0 $ | 1000 | XFRMR LAMINATED 12VA CHAS... |
28A2025-000 | Laird-Signal... | 0.36 $ | 1000 | FERRITE CORE HINGEDHinged... |
28A2026-0A2 | Laird-Signal... | 0.99 $ | 18864 | FERRITE CORE 270 OHM HING... |
241-5-28A26 | Pulse Electr... | 0.0 $ | 1000 | XFRMR LAMINATED 12VA CHAS... |
28A2827-0A2 | Laird-Signal... | 20.91 $ | 1000 | FCCRND,SPL,BB,CSBL 72X39X... |
28A2026-0A0 | Laird-Signal... | 0.43 $ | 1000 | FERRITE CORE HINGEDHinged... |
28A2913-0A2 | Laird-Signal... | 1.19 $ | 2881 | FERRITE CORE 177 OHM HING... |
28A2024-0A2 | Laird-Signal... | 1.99 $ | 14061 | FERRITE CORE 280 OHM HING... |
28A2809-0A2 | Laird-Signal... | 1.39 $ | 17024 | FERRITE CORE 220 OHM HING... |
28A2005-0A2 | Laird-Signal... | 0.53 $ | 1061 | FERRITE CORE 190 OHM HING... |
28A2738-0A2 | Laird-Signal... | 1.22 $ | 3765 | FERRITE CORE 233 OHM HING... |
28A2307-0A2 | Laird-Signal... | 0.88 $ | 1000 | FERRITE CORE 183 OHM HING... |
28A2029-0A0 | Laird-Signal... | 1.18 $ | 31643 | FERRITE CORE 250 OHM HING... |
28A2025-0A0 | Laird-Signal... | 0.92 $ | 11825 | FERRITE CORE 320 OHM HING... |
WFB0-28A22P-CD-F0 | ITT Cannon, ... | 389.42 $ | 1000 | CONN CIRCULARPosition Cir... |
28A2029-0A2 | Laird-Signal... | 1.18 $ | 32892 | FERRITE CORE 250 OHM HING... |
28A2736-000 | Laird-Signal... | 0.36 $ | 1000 | FERRITE CORE HINGEDHinged... |
28A2025-0A2 | Laird-Signal... | 0.92 $ | 15889 | FERRITE CORE 320 OHM HING... |
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