Allicdata Part #: | WVL9FJ820K-ND |
Manufacturer Part#: |
WVL9FJ820K |
Price: | $ 0.00 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | WVL 82 10% F09 |
More Detail: | 82µH Adjustable Inductor 84 @ 2.5MHz Radial, Verti... |
DataSheet: | WVL9FJ820K Datasheet/PDF |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | WVL |
Part Status: | Obsolete |
Inductance: | 82µH |
Tolerance: | ±10% |
Q @ Freq: | 84 @ 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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Adjustable Inductors are electrical components that can be used to adjust the amount of inductance in a particular circuit. This is achieved by adjusting the core material, wire type, and number of turns of a coil within the inductor. The WVL9FJ820K is an adjustable inductor able to do just that.
The WVL9FJ820K is a variable inductor that can be adjusted to fit the needs of many applications. It works by being wound around an adjustable core, with each layer of wiring allowing for more or less inductance to be obtained. The adjustable core is made up of two components – a ferrite core and a ceramic bobbin, which are arranged in a specific manner to allow for the changing of the inductance.
The WVL9FJ820K is mainly used in the fields of radio receivers and high frequency amplifiers. Its adjustable core allows for a precise control of the inductance value, which can be adjusted to conform to different frequencies being sent through the components. This makes it an ideal choice when accuracy of the inductance is needed or desired. Other applications for this adjustable inductor include power supplies, digital signal processing, switching power supplies, and pulse circuits.
The working principle of the WVL9FJ820K is based on magnetic flux. Magnetic flux is the result of the electric current flowing through the inductor, as well as the magnetic field that is created by the coil. By adjusting the core, the amount of flux in the inductor can be adjusted, in turn affecting the amount of inductance that is obtained.
By varying the core material, wire type, and number of turns, the WVL9FJ820K can be adjusted to meet the specific requirements of a given application. With its adjustable core, the inductance can be precisely controlled, giving users the flexibility to adapt the inductor to meet the needs of the circuit.
In conclusion, the WVL9FJ820K is a variable inductor designed to adjust the amount of inductance in a particular circuit. Its adjustable core facilitates precision control, allowing it to be used in radio receivers, high frequency amplifiers, and other applications requiring exact tuning. By varying the core material, wire type, and number of turns, the inductance can be adapted to meet the specific requirements of the application at hand.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
WVL9EB120K | Vishay Dale | 0.0 $ | 1000 | WVL 12 10% EB E212H Adjus... |
WVL9EB180K | Vishay Dale | 0.0 $ | 1000 | WVL 18 10% EB E218H Adjus... |
WVL9EB1R0J | Vishay Dale | 0.0 $ | 1000 | WVL 1 5% EB E21H Adjustab... |
WVL9EB1R2K | Vishay Dale | 0.0 $ | 1000 | WVL 1.2 10% EB E21.2H Adj... |
WVL9EB1R5K | Vishay Dale | 0.0 $ | 1000 | WVL 1.5 10% EB E21.5H Adj... |
WVL9EB1R8K | Vishay Dale | 0.0 $ | 1000 | WVL 1.8 10% EB E21.8H Adj... |
WVL9EB270K | Vishay Dale | 0.0 $ | 1000 | WVL 27 10% EB E227H Adjus... |
WVL9EB2R2K | Vishay Dale | 0.0 $ | 1000 | WVL 2.2 10% EB E22.2H Adj... |
WVL9EB2R7K | Vishay Dale | 0.0 $ | 1000 | WVL 2.7 10% EB E22.7H Adj... |
WVL9EB330K | Vishay Dale | 0.0 $ | 1000 | WVL 33 10% EB E233H Adjus... |
WVL9EB3R9K | Vishay Dale | 0.0 $ | 1000 | WVL 3.9 10% EB E23.9H Adj... |
WVL9EB561K | Vishay Dale | 0.0 $ | 1000 | WVL 560 10% EB E2Adjustab... |
WVL9EB5R6K | Vishay Dale | 0.0 $ | 1000 | WVL 5.6 10% EB E25.6H Adj... |
WVL9EB8R2K | Vishay Dale | 0.0 $ | 1000 | WVL 8.2 10% EB E28.2H Adj... |
WVL9FJ100K | Vishay Dale | 0.0 $ | 1000 | WVL 10 10% F0910H Adjusta... |
WVL9FJ101K | Vishay Dale | 0.0 $ | 1000 | WVL 100 10% F09100H Adjus... |
WVL9FJ102K | Vishay Dale | 0.0 $ | 1000 | WVL 1K 10% F091mH Adjusta... |
WVL9FJ103K | Vishay Dale | 0.0 $ | 1000 | WVL 10K 10% F0910mH Adjus... |
WVL9FJ104K | Vishay Dale | 0.0 $ | 1000 | WVL 100K 10% F09100mH Adj... |
WVL9FJ120K | Vishay Dale | 0.0 $ | 1000 | WVL 12 10% F0912H Adjusta... |
WVL9FJ121K | Vishay Dale | 0.0 $ | 1000 | WVL 120 10% F09120H Adjus... |
WVL9FJ122K | Vishay Dale | 0.0 $ | 1000 | WVL 1.2K 10% F091.2mH Adj... |
WVL9FJ123K | Vishay Dale | 0.0 $ | 1000 | WVL 12K 10% F0912mH Adjus... |
WVL9FJ150K | Vishay Dale | 0.0 $ | 1000 | WVL 15 10% F0915H Adjusta... |
WVL9FJ151K | Vishay Dale | 0.0 $ | 1000 | WVL 150 10% F09150H Adjus... |
WVL9FJ152K | Vishay Dale | 0.0 $ | 1000 | WVL 1.5K 10% F091.5mH Adj... |
WVL9FJ153K | Vishay Dale | 0.0 $ | 1000 | WVL 15K 10% F0915mH Adjus... |
WVL9FJ180K | Vishay Dale | 0.0 $ | 1000 | WVL 18 10% F0918H Adjusta... |
WVL9FJ181K | Vishay Dale | 0.0 $ | 1000 | WVL 180 10% F09180H Adjus... |
WVL9FJ182K | Vishay Dale | 0.0 $ | 1000 | WVL 1.8K 10% F091.8mH Adj... |
WVL9FJ1R0J | Vishay Dale | 0.0 $ | 1000 | WVL 1 5% F091H Adjustable... |
WVL9FJ1R0K | Vishay Dale | 0.0 $ | 1000 | WVL 1 10% F091H Adjustabl... |
WVL9FJ1R2K | Vishay Dale | 0.0 $ | 1000 | WVL 1.2 10% F091.2H Adjus... |
WVL9FJ1R5K | Vishay Dale | 0.0 $ | 1000 | WVL 1.5 10% F091.5H Adjus... |
WVL9FJ1R8K | Vishay Dale | 0.0 $ | 1000 | WVL 1.8 10% F091.8H Adjus... |
WVL9FJ220K | Vishay Dale | 0.0 $ | 1000 | WVL 22 10% F0922H Adjusta... |
WVL9FJ221K | Vishay Dale | 0.0 $ | 1000 | WVL 220 10% F09220H Adjus... |
WVL9FJ222K | Vishay Dale | 0.0 $ | 1000 | WVL 2.2K 10% F092.2mH Adj... |
WVL9FJ223K | Vishay Dale | 0.0 $ | 1000 | WVL 22K 10% F0922mH Adjus... |
WVL9FJ270K | Vishay Dale | 0.0 $ | 1000 | WVL 27 10% F0927H Adjusta... |
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