Allicdata Part #: | IM10RFCMBH820J13-ND |
Manufacturer Part#: |
IM10RFCMBH820J13 |
Price: | $ 4.50 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | IM-10RFCM-13 82 5% B08 |
More Detail: | 82µH Unshielded Molded Inductor 220mA 6.2 Ohm Max ... |
DataSheet: | IM10RFCMBH820J13 Datasheet/PDF |
Quantity: | 1000 |
50 +: | $ 4.05216 |
100 +: | $ 3.92553 |
500 +: | $ 3.67227 |
1000 +: | $ 3.36836 |
Q @ Freq: | 65 @ 800kHz |
Height - Seated (Max): | -- |
Size / Dimension: | 0.250" Dia x 0.600" L (6.35mm x 15.24mm) |
Supplier Device Package: | Axial |
Package / Case: | Axial |
Mounting Type: | Through Hole |
Features: | -- |
Inductance Frequency - Test: | 800kHz |
Operating Temperature: | -55°C ~ 125°C |
Ratings: | -- |
Frequency - Self Resonant: | 2MHz |
Series: | IM-10RFCM-13 |
DC Resistance (DCR): | 6.2 Ohm Max |
Shielding: | Unshielded |
Current - Saturation: | -- |
Current Rating: | 220mA |
Tolerance: | ±5% |
Inductance: | 82µH |
Material - Core: | Iron |
Type: | Molded |
Part Status: | Active |
Packaging: | -- |
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Fixed inductors, such as the IM10RFCMBH820J13, are passive electrical components used in electronic circuits to create legible oscillations and store energy. By adjusting parameters such as capacitance and inductance, inductors can filter and attenuate signals, regulate current flow, or provide heavy current paths. They are extensively used in a variety of applications ranging from analog radio systems to digital switching circuits.
The IM10RFCMBH820J13 is a heat-resistant, high-voltage-resistant, and low-profile fixed inductor. It was primarily designed for use in power supplies and digital circuits, but can be applied in a multitude of applications. In its simplest form, it is composed of an insulated coil of wire, commonly made from a copper or aluminum alloy, with a length of several dozen millimeters and a diameter that varies from three to ten millimeters. The purpose of this coil is to create a loop that builds and stores energy in the presence of an electromagnetic field, primarily generated by the current of an alternating wave.
The working principle of the IM10RFCMBH820J13 is based on Faraday’s Law of Induction, which states that when a conductor moves through a magnetic field, an electric current is induced in it. In the case of the IM10RFCMBH820J13, the coil of wire is located between two magnets, which creates a magnetic field. When an alternating current is applied, it proBelects the wire and induces an electric current. This alternating current eventually creates an oscillating magnetic field that alternates in polarity. The interaction between these two fields stores energy in the coil.
The IM10RFCMBH820J13 can store large amounts of energy in a small space, and because of this, has found its use in a wide array of electronic applications. It is commonly used in power supplies to filter and improve the quality of the system’s output, provide power isolation, and also protect the circuit from electromagnetic interference. It is also used as a matching component for amplifiers, in order to provide stabilization, and as a noise suppressor. Additionally, the IM10RFCMBH820J13 can be used for signal processing applications such as transducers, encoders, and signal transceivers, as well as in medical equipment to improve system accuracy and sensitivity.
The IM10RFCMBH820J13 is a versatile, fixed inductor with a range of applications. It is designed to provide significant energy storage and filtering capabilities, allowing engineers and circuit designers to create reliable and robust electronic circuits and systems. By leveraging Faraday’s Law of Induction, the IM10RFCMBH820J13 is capable of significantly improving power quality, signal reliability, and system accuracy.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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IM10RFCLEZ103J12 | Vishay Dale | 2.89 $ | 1000 | IM-10RFCL-12 10K 5% EZ E2... |
IM10RFCMEZ120J13 | Vishay Dale | 2.99 $ | 1000 | IM-10RFCM-13 12 5% EZ E21... |
IM10RFCLEZ4R7K12 | Vishay Dale | 3.12 $ | 1000 | IM-10RFCL-12 4.7 10% EZ E... |
IM10RFCLRA101K12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 100 10% RB51... |
IM10RFCLRA1R8K12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 1.8 10% RB51... |
IM10RFCLRA220K12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 22 10% RB522... |
IM10RFCLRA221J12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 220 5% RB522... |
IM10RFCLRA3R3K12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 3.3 10% RB53... |
IM10RFCLRA4R7K12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 4.7 10% RB54... |
IM10RFCLRA6R8K12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 6.8 10% RB56... |
IM10RFCLSK220K12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 22 10% RJ322... |
IM10RFCLSK221J12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 220 5% RJ322... |
IM10RFCLSK4R7K12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 4.7 10% RJ34... |
IM10RFCLSK6R8K12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 6.8 10% RJ36... |
IM10RFCMBH100K13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 10 10% B0810... |
IM10RFCMBH101J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 100 5% B0810... |
IM10RFCMBH102J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 1K 5% B081mH... |
IM10RFCMBH120K13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 12 10% B0812... |
IM10RFCMBH121J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 120 5% B0812... |
IM10RFCMBH122J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 1.2K 5% B081... |
IM10RFCMBH150K13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 15 10% B0815... |
IM10RFCMBH151J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 150 5% B0815... |
IM10RFCMBH220K13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 22 10% B0822... |
IM10RFCMBH222J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 2.2K 5% B082... |
IM10RFCMBH270J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 27 5% B0827H... |
IM10RFCMBH330J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 33 5% B0833H... |
IM10RFCMBH330K13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 33 10% B0833... |
IM10RFCMBH331J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 330 5% B0833... |
IM10RFCMBH390K13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 39 10% B0839... |
IM10RFCMBH470J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 47 5% B0847H... |
IM10RFCMBH471J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 470 5% B0847... |
IM10RFCMBH4R7K13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 4.7 10% B084... |
IM10RFCMBH560J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 56 5% B0856H... |
IM10RFCMBH561J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 560 5% B0856... |
IM10RFCMBH5R6K13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 5.6 10% B085... |
IM10RFCMBH6R8K13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 6.8 10% B086... |
IM10RFCMBH820J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 82 5% B0882H... |
IM10RFCMBH8R2K13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 8.2 10% B088... |
IM10RFCMEB5R6K13 | Vishay Dale | 4.66 $ | 1000 | IM-10RFCM-13 5.6 10% EB E... |
IM10RFCMBH111J13 | Vishay Dale | 4.95 $ | 1000 | IM-10RFCM-13 110 5% B0811... |
FIXED IND 10UH 590MA 350 MOHM10H Unshiel...
FIXED IND 22NH 1.4A 70 MOHM SMD22nH Unsh...
FIXED IND 13NH 600MA SMD13nH Unshielded ...
FIXED IND 680UH 210MA 4.6 OHM680H Unshie...
FIXED IND 470UH 1.3A 280 MOHM TH470H Uns...
FIXED IND 8.2UH 165MA 2.2 OHM TH8.2H Uns...