
Allicdata Part #: | WVL9EB8R2K-ND |
Manufacturer Part#: |
WVL9EB8R2K |
Price: | $ 0.00 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | WVL 8.2 10% EB E2 |
More Detail: | 8.2µH Adjustable Inductor 76 @ 7.9MHz Radial, Vert... |
DataSheet: | ![]() |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | WVL |
Part Status: | Obsolete |
Inductance: | 8.2µH |
Tolerance: | ±10% |
Q @ Freq: | 76 @ 7.9MHz |
Mounting Type: | Through Hole |
Package / Case: | Radial, Vertical Cylinder |
Size / Dimension: | 0.300" Dia (7.62mm) |
Height: | 0.430" (10.92mm) |
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The WVL9EB8R2K Adjustable Inductor features an adjustable range and optimized Q factor, making it a great option for a wide range of applications and designs. The inductor uses a unique, patented technology to enable the high-frequency, fine-tuning and linearization of the inductance. This adjustable range typically ranges from 10mH-20mH. It also features a maximum DCR of 25 mΩ and a peak current rating of 2.4A r.m.s.
This type of adjustable inductor is often used for radio-frequency signal filtering applications, for matching and transforming high-frequency signals and impedances. The adjustable inductor also provides excellent high-frequency performance for issues such as antenna matching. Other applications include ferrite bead attenuators, impedance matching with transformers and impedance matching to integrated circuit packages.
The WVL9EB8R2K adjustable inductor includes a patented high-frequency tuning and linearization. This allows for both a wide range of inductances to be tuned in the same package, as well as for fine-tuning. This makes it ideal for radio-frequency signal filtering applications. Additionally, the inductor\'s high-frequency performance is significantly improved, making it an ideal choice for applications such as antenna matching.
The adjustable inductor has a wide range of advantages over traditional inductors. It has a low parasitic inductance, making it ideal for matching and transforming high-frequency signals. Additionally, its adjustable range and high-frequency performance make it ideal for applications such as waveform filtration. Traditional inductors often experience losses in high-frequency applications due to parasitic inductances, but the adjustable inductor is unaffected by this.
An adjustable inductor works by allowing the magnetic field to flow through its windings. This creates an inductance which can then be varied by adjusting the tuning parameters of the device. This is achieved by using different types of capacitors, or by adjusting the number of turns in the windings. By changing the inductance, the device is able to filter out an undesired frequency, allowing it to be more useful for radio-frequency signal filtering applications. It can also be used to match impedances between different components, allowing for improved efficiency and performance.
The WVL9EB8R2K adjustable inductor is perfect for radio-frequency signal filtering applications, as well as for matching and transforming high-frequency signals and impedances. Its adjustable range and optimized Q factor enable it to be used for a wide range of applications and designs. It also features a high-frequency tuning and linearization feature, making it an ideal choice for antenna matching applications. Additionally, its low parasitic inductance makes it an ideal choice for applications such as waveform filtration. The WVL9EB8R2K adjustable inductor is truly an excellent choice for a wide variety of applications.
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Part Number | Manufacturer | Price | Quantity | Description |
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WVL9FJR22J | Vishay Dale | 0.0 $ | 1000 | WVL .22 5% F09220nH Adjus... |
WVL9EB1R2K | Vishay Dale | 0.0 $ | 1000 | WVL 1.2 10% EB E21.2H Adj... |
WVL9FJ103K | Vishay Dale | 0.0 $ | 1000 | WVL 10K 10% F0910mH Adjus... |
WVL9FJ123K | Vishay Dale | 0.0 $ | 1000 | WVL 12K 10% F0912mH Adjus... |
WVL9FJ121K | Vishay Dale | 0.0 $ | 1000 | WVL 120 10% F09120H Adjus... |
WVL9FJ122K | Vishay Dale | 0.0 $ | 1000 | WVL 1.2K 10% F091.2mH Adj... |
WVL9FJ822K | Vishay Dale | 0.0 $ | 1000 | WVL 8.2K 10% F098.2mH Adj... |
WVL9FJR22JH | Vishay Dale | 0.0 $ | 1000 | WVL-H .22 5% F09220nH Adj... |
WVL9FJR10J | Vishay Dale | 0.0 $ | 1000 | WVL .1 5% F09100nH Adjust... |
WVL9FJR15J | Vishay Dale | 0.0 $ | 1000 | WVL .15 5% F09150nH Adjus... |
WVL9EB180K | Vishay Dale | 0.0 $ | 1000 | WVL 18 10% EB E218H Adjus... |
WVL9EB561K | Vishay Dale | 0.0 $ | 1000 | WVL 560 10% EB E2Adjustab... |
WVL9FJ682K | Vishay Dale | 0.0 $ | 1000 | WVL 6.8K 10% F096.8mH Adj... |
WVL9FJ681K | Vishay Dale | 0.0 $ | 1000 | WVL 680 10% F09680H Adjus... |
WVL9FJR47JH | Vishay Dale | 0.0 $ | 1000 | WVL-H .47 5% F09470nH Adj... |
WVL9FJR27J | Vishay Dale | 0.0 $ | 1000 | WVL .27 5% F09270nH Adjus... |
WVL9FJ472K | Vishay Dale | 0.0 $ | 1000 | WVL 4.7K 10% F094.7mH Adj... |
WVL9FJ330K | Vishay Dale | 0.0 $ | 1000 | WVL 33 10% F0933H Adjusta... |
WVL9FJ100K | Vishay Dale | 0.0 $ | 1000 | WVL 10 10% F0910H Adjusta... |
WVL9FJ392K | Vishay Dale | 0.0 $ | 1000 | WVL 3.9K 10% F093.9mH Adj... |
WVL9EB330K | Vishay Dale | 0.0 $ | 1000 | WVL 33 10% EB E233H Adjus... |
WVL9FJ1R8K | Vishay Dale | 0.0 $ | 1000 | WVL 1.8 10% F091.8H Adjus... |
WVL9FJ272K | Vishay Dale | 0.0 $ | 1000 | WVL 2.7K 10% F092.7mH Adj... |
WVL9EB8R2K | Vishay Dale | 0.0 $ | 1000 | WVL 8.2 10% EB E28.2H Adj... |
WVL9FJ151K | Vishay Dale | 0.0 $ | 1000 | WVL 150 10% F09150H Adjus... |
WVL9FJ1R5K | Vishay Dale | 0.0 $ | 1000 | WVL 1.5 10% F091.5H Adjus... |
WVL9FJR56J | Vishay Dale | 0.0 $ | 1000 | WVL .56 5% F09560nH Adjus... |
WVL9FJ181K | Vishay Dale | 0.0 $ | 1000 | WVL 180 10% F09180H Adjus... |
WVL9FJ390K | Vishay Dale | 0.0 $ | 1000 | WVL 39 10% F0939H Adjusta... |
WVL9FJ473K | Vishay Dale | 0.0 $ | 1000 | WVL 47K 10% F0947mH Adjus... |
WVL9EB1R8K | Vishay Dale | 0.0 $ | 1000 | WVL 1.8 10% EB E21.8H Adj... |
WVL9FJ3R9K | Vishay Dale | 0.0 $ | 1000 | WVL 3.9 10% F093.9H Adjus... |
WVL9FJ562K | Vishay Dale | 0.0 $ | 1000 | WVL 5.6K 10% F095.6mH Adj... |
WVL9FJ180K | Vishay Dale | 0.0 $ | 1000 | WVL 18 10% F0918H Adjusta... |
WVL9FJ8R2K | Vishay Dale | 0.0 $ | 1000 | WVL 8.2 10% F098.2H Adjus... |
WVL9FJ2R7KH | Vishay Dale | 0.0 $ | 1000 | WVL-H 2.7 10% F092.7H Adj... |
WVL9FJ4R7K | Vishay Dale | 0.0 $ | 1000 | WVL 4.7 10% F094.7H Adjus... |
WVL9FJR18J | Vishay Dale | 0.0 $ | 1000 | WVL .18 5% F09180nH Adjus... |
WVL9EB2R7K | Vishay Dale | 0.0 $ | 1000 | WVL 2.7 10% EB E22.7H Adj... |
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