
Allicdata Part #: | WVL9FJ220K-ND |
Manufacturer Part#: |
WVL9FJ220K |
Price: | $ 0.00 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | WVL 22 10% F09 |
More Detail: | 22µH Adjustable Inductor 100 @ 2.5MHz Radial, Vert... |
DataSheet: | ![]() |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | WVL |
Part Status: | Obsolete |
Inductance: | 22µH |
Tolerance: | ±10% |
Q @ Freq: | 100 @ 2.5MHz |
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 WVL9FJ220K is a type of adjustable inductor renowned for its great performance and wide range of applications. This common electronic component is part of the larger family of energy storage elements known as inductors. It belongs to the class of adjustable inductors because it is designed to be adjustable through physical or electronic means.
Inductors are commonly used to store energy in the form of magnetic fields, and they are used across a variety of electronic applications. Inductors can be used inside of oscillators to regulate and regulate the frequency and amplitude of generated signals. They can also be used as filters, blocking unwanted signals while allowing the desired frequency to pass through. In addition to their widespread use in commercial and technical applications, adjustable inductors are also used in radio, telecom, automotive, and power management applications.
The WVL9FJ220K adjustable inductor meets the demanding needs of electronic design engineers across a variety of industries. It has a maximum inductance of 220 μH, design voltage of 85 V, rated current of 1 A, a size of 12.1 mm x 7 mm, and an inductance range of 5.5-220 μH. The WVL9FJ220K is an encapsulated coil, allowing for increased safety due to its hermetically sealed case. This make it more suitable for use in environments with extreme temperature or humidity.
In its most basic form, the WVL9FJ220K adjustable inductor functions as an energy storage device, able to capture and store energy in the form of a magnetic field. When an external current is passed through it, a more powerful magnetic field is created, which can be used to regulate power and signals. The primary function of the WVL9FJ220K adjustable inductor is to reduce ripple in power supplies, by providing the needed inductance. This can also be used to reduce the noise in audio systems.
The WVL9FJ220K adjustable inductor can also be used in oscillators, where they regulate the amplitude and frequency of signals. This type of adjustable inductor is also useful for filters, where they can block certain frequencies while allowing others to pass through. Additionally, the WVL9FJ220K is suitable for applications such as EMI and RFI filtering. This makes the WVL9FJ220K adjustable inductor a versatile component that can be used for a variety of applications.
In order to alter the inductance of the WVL9FJ220K adjustable inductor, there are three primary methods of adjustment. The first is through physical adjustment, where the user is able to adjust the inductance manually by turning the dial on the outside of the device. The second is through electronic adjustment, where a control signal is used to adjust the inductance. The third is through the use of mechanical controls, where the user is able to adjust the inductance through the use of levers or pulleys.
The WVL9FJ220K adjustable inductor is a reliable and versatile component, suitable for a wide range of applications. It is part of the family of adjustable inductors, and as the name suggests, it is designed to be adjustable to suit different power needs. Whether used in a power supply, oscillator, filter, or other electronic application, the WVL9FJ220K adjustable inductor is sure to provide years of reliable performance.
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WVL9FJ121K | Vishay Dale | 0.0 $ | 1000 | WVL 120 10% F09120H Adjus... |
WVL9FJ122K | Vishay Dale | 0.0 $ | 1000 | WVL 1.2K 10% F091.2mH Adj... |
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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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