
Allicdata Part #: | IM10RFCLRA101K12-ND |
Manufacturer Part#: |
IM10RFCLRA101K12 |
Price: | $ 3.21 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | IM-10RFCL-12 100 10% RB5 |
More Detail: | 100µH Shielded Molded Inductor 400mA 3.2 Ohm Max A... |
DataSheet: | ![]() |
Quantity: | 1000 |
250 +: | $ 2.88288 |
500 +: | $ 2.79279 |
1000 +: | $ 2.61261 |
Q @ Freq: | 100 @ 1.5MHz |
Height - Seated (Max): | -- |
Size / Dimension: | 0.310" Dia x 0.900" L (7.87mm x 22.86mm) |
Supplier Device Package: | Axial |
Package / Case: | Axial |
Mounting Type: | Through Hole |
Features: | -- |
Inductance Frequency - Test: | 1.5MHz |
Operating Temperature: | -55°C ~ 125°C |
Ratings: | -- |
Frequency - Self Resonant: | 13MHz |
Series: | IM-10RFCL-12 |
DC Resistance (DCR): | 3.2 Ohm Max |
Shielding: | Shielded |
Current - Saturation: | -- |
Current Rating: | 400mA |
Tolerance: | ±5% |
Inductance: | 100µH |
Material - Core: | Iron |
Type: | Molded |
Part Status: | Active |
Packaging: | -- |
Due to market price fluctuations, if you need to purchase or consult the price. You can contact us or emial to us: sales@allicdata.com
Fixed inductors are regarded as basic elements for many electrical circuits. An essentialcomponent of the electronic system, IM10RFCLRA101K12 is one of the most widely used inductors on the market today. This inductor is not only versatile and reliable, but also enables circuitfunctionality in many applications.
The main purpose of an inductor is to store energy in a magnetic field. In its simplest terms,an inductor consists of a core material, such as a ferrite, and a conductor coil surrounding thecore. When electrical current is passed through the conductor coil, a magnetic field is createdaround the core, which stores the energy.
The IM10RFCLRA101K12 is an innovative type of fixed inductor designed for applications involving high frequency. This inductor has an inductance range of 1μH-40μH and anoperating temperature range of -20 to 105˚C. It features a robust construction that ensures anaccurate direct current (DC) to alternating current (AC) conversion. This makes it suitable forapplications in fields such as power supply systems, motor control systems, and other deviceswhich require high efficiency and reliability.
The inductor is made of an externally applied magnetic field that is created by a coil formedfrom solid wire. This type of inductor can deliver higher inductance values than similardevices due to its efficient flux transfer and improved inductance-to-current ratio. It offers anexcellent combination of low resistance and high inductance with minimal distortion producedby the core materials, which means that it can be used for both AC and DC current.
The work principle of the IM10RFCLRA101K12 fixed inductor is based on Faraday’s Law ofElectromagnetic Induction. The core material, along with the wire, create a changingmagnetic field around the device as current is applied to it. This changing magnetic fieldcauses a current to be induced in the inductor, which makes the inductor circuit operational.
The IM10RFCLRA101K12 inductor can be used in a wide variety of applications, such asaudio/video electronics, DC/DC converters, AC/DC converters, and switching power supplies.It is also suitable for use in high-frequency telecommunication circuits, in which it canhandle power with minimal distortion.
In summary, the IM10RFCLRA101K12 inductor is an excellent choice for a variety ofapplications. It offers a reliable, high-efficiency performance, with minimal distortion andlow inductance-to-current ratio. The inductor is robust and easy to use, making it ideal formany types of electronic systems.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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IM10RFCMEZ102J13 | Vishay Dale | 2.11 $ | 1000 | IM-10RFCM-13 1K 5% EZ E21... |
IM10RFCMBH3R9K13 | Vishay Dale | 5.47 $ | 1000 | IM-10RFCM-13 3.9 10% B083... |
IM10RFCMRA1R0K13 | Vishay Dale | 2.57 $ | 1000 | IM-10RFCM-13 1 10% RB51H ... |
IM10RFCMBH820J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 82 5% B0882H... |
IM10RFCLEB103J12 | Vishay Dale | 6.1 $ | 1000 | IM-10RFCL-12 10K 5% EB E2... |
IM10RFCMBH111J13 | Vishay Dale | 4.95 $ | 1000 | IM-10RFCM-13 110 5% B0811... |
IM10RFCMBH102J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 1K 5% B081mH... |
IM10RFCMRA2R2K13 | Vishay Dale | 2.57 $ | 1000 | IM-10RFCM-13 2.2 10% RB52... |
IM10RFCMBH4R7K13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 4.7 10% B084... |
IM10RFCLBH472J12 | Vishay Dale | 6.29 $ | 1000 | IM-10RFCL-12 4.7K 5% B084... |
IM10RFCLBH1R0K12 | Vishay Dale | 6.59 $ | 1000 | IM-10RFCL-12 1 10% B081H ... |
IM10BH822J | Vishay Dale | 0.0 $ | 1000 | IM-10 8.2K 5% B088.2mH Un... |
IM10BH103K | Vishay Dale | 0.0 $ | 1000 | IM-10 10K 10% B0810mH Uns... |
IM10RFCMBH121J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 120 5% B0812... |
IM10RFCLBH8R2K12 | Vishay Dale | 6.59 $ | 1000 | IM-10RFCL-12 8.2 10% B088... |
IM10RFCLEB6R8K12 | Vishay Dale | 6.42 $ | 1000 | IM-10RFCL-12 6.8 10% EB E... |
IM10BH472J | Vishay Dale | 0.0 $ | 1000 | IM-10 4.7K 5% B084.7mH Un... |
IM10RFCMEZ5R6K13 | Vishay Dale | 2.11 $ | 1000 | IM-10RFCM-13 5.6 10% EZ E... |
IM10RFCMBH1R2K13 | Vishay Dale | 5.47 $ | 1000 | IM-10RFCM-13 1.2 10% B081... |
IM10RFCMBH1R0K13 | Vishay Dale | 5.47 $ | 1000 | IM-10RFCM-13 1 10% B081H ... |
IM10RFCMEZ8R2K13 | Vishay Dale | 2.11 $ | 1000 | IM-10RFCM-13 8.2 10% EZ E... |
IM10RFCLSK6R8K12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 6.8 10% RJ36... |
IM10RFCLSK221J12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 220 5% RJ322... |
IM10RFCLBH1R0J12 | Vishay Dale | 8.75 $ | 1000 | IM-10RFCL-12 1 5% B081H S... |
IM10RFCLEZ103J12 | Vishay Dale | 2.89 $ | 1000 | IM-10RFCL-12 10K 5% EZ E2... |
IM10RFCMBH1R8K13 | Vishay Dale | 5.47 $ | 1000 | IM-10RFCM-13 1.8 10% B081... |
IM10RFCLRA6R8K12 | Vishay Dale | 3.21 $ | 1000 | IM-10RFCL-12 6.8 10% RB56... |
IM10RFCMBH151J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 150 5% B0815... |
IM10RFCMEB3R3K13 | Vishay Dale | 5.5 $ | 1000 | IM-10RFCM-13 3.3 10% EB E... |
IM10RFCLBH3R3K12 | Vishay Dale | 6.59 $ | 1000 | IM-10RFCL-12 3.3 10% B083... |
IM10BH822K | Vishay Dale | 0.0 $ | 1000 | IM-10 8.2K 10% B088.2mH U... |
IM10RFCLEB4R7K12 | Vishay Dale | 6.42 $ | 1000 | IM-10RFCL-12 4.7 10% EB E... |
AQCD3-IM100/240VAC | Panasonic El... | 10.72 $ | 175 | MOD AC INPUT 100/240VAC 4... |
IM10RA822J | Vishay Dale | 0.0 $ | 1000 | IM-10 8.2K 5% RB58.2mH Un... |
IM10RFCMEZ3R9K13 | Vishay Dale | 2.51 $ | 1000 | IM-10RFCM-13 3.9 10% EZ E... |
IM10RFCMBH470J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 47 5% B0847H... |
IM10RFCLBH1R2K12 | Vishay Dale | 6.59 $ | 1000 | IM-10RFCL-12 1.2 10% B081... |
IM10BH682J | Vishay Dale | 0.0 $ | 1000 | IM-10 6.8K 5% B086.8mH Un... |
IM10RFCLBH680J12 | Vishay Dale | 6.59 $ | 1000 | IM-10RFCL-12 68 5% B0868H... |
IM10RFCMEZ120J13 | Vishay Dale | 2.99 $ | 1000 | IM-10RFCM-13 12 5% EZ E21... |
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...
