Allicdata Part #: | WVL9FJ391K-ND |
Manufacturer Part#: |
WVL9FJ391K |
Price: | $ 0.00 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | WVL 390 10% F09 |
More Detail: | 390µH Adjustable Inductor 80 @ 790kHz Radial, Vert... |
DataSheet: | WVL9FJ391K Datasheet/PDF |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | WVL |
Part Status: | Obsolete |
Inductance: | 390µH |
Tolerance: | ±10% |
Q @ Freq: | 80 @ 790kHz |
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 the electronic components used to give inductance to electrical circuits, such as DC power supplies, loudspeakers, and RF receivers. As its name suggests, adjustable inductors have adjustable values, allowing the user to tune the output to a specific lower or higher inductance, depending on the desired application. WVL9FJ391K is an adjustable inductor manufactured by Wuhan Victor Technology and is a popular component used in high-frequency applications due to its superior performance. This article will discuss the application field and working principle of WVL9FJ391K.
WVL9FJ391K is an adjustable inductor composed of a circular steel core wrapped with a copper coil. It features three fixed terminals and two adjustable ones, which is different from a conical or cylindrical coil inductor. The two adjustable terminals, when adjusted, can provide the inductance value needed for the circuit. This adjustable inductor is typically used in applications where resistance or inductance values need to be adjusted so as to optimize the design of the circuit, such as antenna tuning.
As for the application field of WVL9FJ391K, it is mainly used in high-frequency applications because it provides superior performance compared to other inductors. Due to its unique construction, it can provide increased inductance values without needing a large coil and occupies less space. Its adjustable construction also enables it to be modified to better match the desired output power levels of various applications such as RF amplifiers and antenna systems. Additionally, it is used in multi-layer PCBs in order to reduce the circuit\'s layout space to a minimum and maximize space efficiency.
The working principle of WVL9FJ391K is based on Faraday\'s Law of Electromagnetic Induction. As current passes through the inductor\'s core, it creates a magnetic field. This magnetic field causes a sensing current to flow through the wire, which then causes a change in the inductance value. This change in inductance is then used to modify the current passing through the circuit, which can be used to regulate the power and signal levels for a given application.
By varying the inductance value of WVL9FJ391K, it is possible to attain a variety of frequencies. This feature makes it ideal for applications that need to operate at any frequency within a given range. Furthermore, the adjustable construction of this inductor enables users to easily tune it to the desired output power levels with minimal effort. Additionally, it has a wide frequency range and high isolation between the primary and secondary windings, further increasing its usefulness as a high-frequency component.
In conclusion, WVL9FJ391K is an adjustable inductor manufactured by Wuhan Victor Technology used in high-frequency applications. It features a unique construction that allows for the inductance value to be adjusted easily, enabling users to modify the current passing through the circuit and regulate the power and signal levels for a given application. Its adjustable construction and wide frequency range make WVL9FJ391K a great component for applications that require high-frequency capabilities.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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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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