Allicdata Part #: | IM10RFCLSK221J12-ND |
Manufacturer Part#: |
IM10RFCLSK221J12 |
Price: | $ 3.21 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | IM-10RFCL-12 220 5% RJ3 |
More Detail: | 220µH Shielded Molded Inductor 200mA 12 Ohm Max Ax... |
DataSheet: | IM10RFCLSK221J12 Datasheet/PDF |
Quantity: | 1000 |
400 +: | $ 2.88288 |
800 +: | $ 2.70270 |
1200 +: | $ 2.61261 |
Q @ Freq: | 95 @ 1MHz |
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: | 1MHz |
Operating Temperature: | -55°C ~ 125°C |
Ratings: | -- |
Frequency - Self Resonant: | 9MHz |
Series: | IM-10RFCL-12 |
DC Resistance (DCR): | 12 Ohm Max |
Shielding: | Shielded |
Current - Saturation: | -- |
Current Rating: | 200mA |
Tolerance: | ±5% |
Inductance: | 220µH |
Material - Core: | Iron |
Type: | Molded |
Part Status: | Active |
Packaging: | -- |
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Fixed inductors, also known as non-variable inductors, are electrical components designed to provide a fixed inductance to an electrical circuit. By definition, the inductor opposes the flow of current through it. The IM10RFCLSK221J12 is a fixed inductor that is mainly used in power supplies, dc-dc converters, bridge rectifiers, electrolytic capacitors, filters, oscillators, and various radio frequencies. Many of these applications are used to reduce voltage instability and protect sensitive electronic devices.
The IM10RFCLSK221J12 is a miniaturized inductor with low DC resistance and high Q-Factor. The low DCR allows it to operate at higher frequencies and operate with less heat. The high Q-Factor makes it well-suited for use in various types of filters. The inductor is designed to provide a low-impedance path for signals up to 10MHz. It also has exceptional stability over temperature changes and extremely low noise.
The working principle of the IM10RFCLSK221J12 fixed inductor is based on the fundamental laws of electromagnetic induction. When a voltage or current is applied to the inductor, an electromagnetic field is generated around it. This field resists the flow of current and induces an electromotive force in the circuit. When the current flowing through the inductor changes, the inductor generates a voltage which opposes the change in current. This is known as inductive reactance.
One of the most important characteristics of fixed inductors is their inductance values, which are determined by the number of turns on the coil. The number of turns can be varied in order to fine-tune the inductance of the inductor. The inductance value of the IM10RFCLSK221J12 is measured in micro-henries and ranges from 1.4 micro-henry to 3.6 micro-henry. This range allows the inductor to be used in a variety of applications such as filters, chokes, and power supplies.
In conclusion, the IM10RFCLSK221J12 is a fixed inductor that is mainly used in power supplies, dc-dc converters, bridge rectifiers, electrolytic capacitors, filters, oscillators, and various radio frequencies. The inductor is designed with low DC resistance and a high Q-Factor, making it ideal for high frequency applications. It also has an adjustable inductance value ranging from 1.4 micro-henrys to 3.6 micro-henrys. The inductor works on the principle of electromagnetic induction and generates a voltage which opposes the flow of current.
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... |
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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... |
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IM10RFCMBH471J13 | Vishay Dale | 4.5 $ | 1000 | IM-10RFCM-13 470 5% B0847... |
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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... |
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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...