Allicdata Part #: | IHB6BV220K-ND |
Manufacturer Part#: |
IHB6BV220K |
Price: | $ 21.78 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | IHB-6 22 10% B40 |
More Detail: | 22µH Unshielded Wirewound Inductor 27.5A 5 mOhm Ma... |
DataSheet: | IHB6BV220K Datasheet/PDF |
Quantity: | 1000 |
16 +: | $ 19.59810 |
112 +: | $ 18.61810 |
Series: | IHB |
Packaging: | -- |
Part Status: | Active |
Type: | Wirewound |
Material - Core: | -- |
Inductance: | 22µH |
Tolerance: | ±10% |
Current Rating: | 27.5A |
Current - Saturation: | -- |
Shielding: | Unshielded |
DC Resistance (DCR): | 5 mOhm Max |
Q @ Freq: | -- |
Frequency - Self Resonant: | -- |
Ratings: | -- |
Operating Temperature: | -55°C ~ 130°C |
Inductance Frequency - Test: | 1kHz |
Features: | -- |
Mounting Type: | Through Hole |
Package / Case: | Radial |
Supplier Device Package: | -- |
Size / Dimension: | 2.000" Dia (50.80mm) |
Height - Seated (Max): | 1.500" (38.10mm) |
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Fixed inductors, also known as chokes or coils, are passive electronic components designed to store energy in the form of a magnetic field when current passes through the component\'s coil. The IHB6BV220K is one such fixed inductor and is designed for a variety of electronic applications. This article will outline the properties of the IHB6BV220K and how it is employed in various applications as well as discussing the working principle of a fixed inductor in general.
Applications of the IHB6BV220K
The IHB6BV220K is a small, surface mount adjustable inductor from an electronic components manufacturer Murata. It is 3320uH rated inductor with a maximum DC current of 200mA. This parts DCR of 0.3 ohm and high shielding factor make it ideally suited to a variety of applications. These include filters for video signals, mobile phone filters, as well as EMI suppression in equipment like smartphones, tablets, and more.
This inductor is also employed for power line noise suppression. It is particularly useful for power supplies with low-noise amplifiers (LNAs) or for applications which require high-speed switching. The IHB6BV220K has a high-precision characteristics which renders it ideal for such applications, as it can maintain a stable and constant inductance value even when a large current is passed through it.
Working Principle of Fixed Inductors
The fundamental principle behind a fixed inductor is the law of induction, discovered by Michael Faraday in 1831. The law states that a current passing through a coil creates a surrounding magnetic field and, inversely, a time varying magnetic field applied to a coil will generate a current in the same coil. This occurs because the changing flux of a magnetic field induces an electromotive force (EMF) in the coil.
When a current is passed through the inductor’s coil, lines of flux will form, with each line like a loop. As they start to move outward, a back-EMF will be formed, opposing the current. This is known as counter-electromotive force and is analogous to the drag forces a rocket experiences as it moves through air and is directly proportional to the rate of change of flux.
Thus, the inductance, L, is equal to the counter-EMF developed which, in turn, produces an opposing force to the current. This EMF forces the current to move slowly, so that over a certain period of time, the flux can build up before dissipating. For a coil with many turns/windings, the resulting EMF is higher, causing a higher counter-electromotive resistance.
A fixed inductor can be thought of as an energy storage device, as it stores energy in the form of a magnetic field. This energy is discharged when the device is no longer energised and it is this mechanism which is employed in many electronic products today to produce the desired results.
Conclusion
The IHB6BV220K is a small, surface mount adjustable inductor from Murata and is ideally suited to a variety of filtering applications. Its high shielding factor, low DCR, and wide inductance range makes it a useful component for applications such as video signal filters, mobile phone filters, power line noise suppression, and more. The IHB6BV220K features high-precision characteristics which allows it to maintain a stable and constant inductance value when a large current is passed through it.
The working principle of a fixed inductor can be explained in terms of Faraday’s law of induction, as it relies on the creation of a magnetic field, when current passes through a coil. The resulting back-EMF generated opposes the current, giving rise to the inductance which, in turn, forces the current to move slowly so that flux can build up over a certain period of time before dissipating. This makes fixed inductors useful for energy storage applications.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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IHB6EB102K | Vishay Dale | 21.14 $ | 1000 | IHB-6 1K 10% EB E21mH Uns... |
IHB6EB103K | Vishay Dale | 21.14 $ | 1000 | IHB-6 10K 10% EB E210mH U... |
IHB6EB123K | Vishay Dale | 21.14 $ | 1000 | IHB-6 12K 10% EB E212mH U... |
IHB6EB150K | Vishay Dale | 21.14 $ | 1000 | IHB-6 15 10% EB E215H Uns... |
IHB6EB183K | Vishay Dale | 21.14 $ | 1000 | IHB-6 18K 10% EB E218mH U... |
IHB6EB220K | Vishay Dale | 21.14 $ | 1000 | IHB-6 22 10% EB E222H Uns... |
IHB6EB221K | Vishay Dale | 21.14 $ | 1000 | IHB-6 220 10% EB E2220H U... |
IHB6EB273K | Vishay Dale | 21.14 $ | 1000 | IHB-6 27K 10% EB E227mH U... |
IHB6EB330K | Vishay Dale | 21.14 $ | 1000 | IHB-6 33 10% EB E233H Uns... |
IHB6EB333K | Vishay Dale | 21.14 $ | 1000 | IHB-6 33K 10% EB E233mH U... |
IHB6EB390K | Vishay Dale | 21.14 $ | 1000 | IHB-6 39 10% EB E239H Uns... |
IHB6EB473K | Vishay Dale | 21.14 $ | 1000 | IHB-6 47K 10% EB E247mH U... |
IHB6EB562K | Vishay Dale | 21.14 $ | 1000 | IHB-6 5.6K 10% EB E25.6mH... |
IHB6EB682K | Vishay Dale | 21.14 $ | 1000 | IHB-6 6.8K 10% EB E26.8mH... |
IHB6EB820K | Vishay Dale | 21.14 $ | 1000 | IHB-6 82 10% EB E282H Uns... |
IHB6BV100K | Vishay Dale | 21.78 $ | 1000 | IHB-6 10 10% B4010H Unshi... |
IHB6BV101K | Vishay Dale | 21.78 $ | 1000 | IHB-6 100 10% B40100H Uns... |
IHB6BV102K | Vishay Dale | 21.78 $ | 1000 | IHB-6 1K 10% B401mH Unshi... |
IHB6BV103K | Vishay Dale | 21.78 $ | 1000 | IHB-6 10K 10% B4010mH Uns... |
IHB6BV121K | Vishay Dale | 21.78 $ | 1000 | IHB-6 120 10% B40120H Uns... |
IHB6BV122K | Vishay Dale | 21.78 $ | 1000 | IHB-6 1.2K 10% B401.2mH U... |
IHB6BV123K | Vishay Dale | 21.78 $ | 1000 | IHB-6 12K 10% B4012mH Uns... |
IHB6BV152K | Vishay Dale | 21.78 $ | 1000 | IHB-6 1.5K 10% B401.5mH U... |
IHB6BV153K | Vishay Dale | 21.78 $ | 1000 | IHB-6 15K 10% B4015mH Uns... |
IHB6BV180K | Vishay Dale | 21.78 $ | 1000 | IHB-6 18 10% B4018H Unshi... |
IHB6BV181K | Vishay Dale | 21.78 $ | 1000 | IHB-6 180 10% B40180H Uns... |
IHB6BV182K | Vishay Dale | 21.78 $ | 1000 | IHB-6 1.8K 10% B401.8mH U... |
IHB6BV183K | Vishay Dale | 21.78 $ | 1000 | IHB-6 18K 10% B4018mH Uns... |
IHB6BV220K | Vishay Dale | 21.78 $ | 1000 | IHB-6 22 10% B4022H Unshi... |
IHB6BV221K | Vishay Dale | 21.78 $ | 1000 | IHB-6 220 10% B40220H Uns... |
IHB6BV222K | Vishay Dale | 21.78 $ | 1000 | IHB-6 2.2K 10% B402.2mH U... |
IHB6BV223K | Vishay Dale | 21.78 $ | 1000 | IHB-6 22K 10% B4022mH Uns... |
IHB6BV270K | Vishay Dale | 21.78 $ | 1000 | IHB-6 27 10% B4027H Unshi... |
IHB6BV271K | Vishay Dale | 21.78 $ | 1000 | IHB-6 270 10% B40270H Uns... |
IHB6BV272K | Vishay Dale | 21.78 $ | 1000 | IHB-6 2.7K 10% B402.7mH U... |
IHB6BV273K | Vishay Dale | 21.78 $ | 1000 | IHB-6 27K 10% B4027mH Uns... |
IHB6BV331K | Vishay Dale | 21.78 $ | 1000 | IHB-6 330 10% B40330H Uns... |
IHB6BV332K | Vishay Dale | 21.78 $ | 1000 | IHB-6 3.3K 10% B403.3mH U... |
IHB6BV333K | Vishay Dale | 21.78 $ | 1000 | IHB-6 33K 10% B4033mH Uns... |
IHB6BV390K | Vishay Dale | 21.78 $ | 1000 | IHB-6 39 10% B4039H Unshi... |
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...