
Allicdata Part #: | WVL9FJ103K-ND |
Manufacturer Part#: |
WVL9FJ103K |
Price: | $ 0.00 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | WVL 10K 10% F09 |
More Detail: | 10mH Adjustable Inductor Radial, Vertical Cylinde... |
DataSheet: | ![]() |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | WVL |
Part Status: | Obsolete |
Inductance: | 10mH |
Tolerance: | ±10% |
Q @ Freq: | -- |
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 among the most common components found in a variety of electronic circuits. The WVL9FJ103K is an adjustable inductor that is widely employed in RF circuits due to its improved performance, dynamic range, and ease of adjustment. In this article, we will discuss the application field and working principle of WVL9FJ103K adjustable inductor.
The WVL9FJ103K is a type of a non-saturating, adjustable inductor that allows the user to easily adjust the inductance value. This is done by physically altering the component\'s turns ratio. Its adjustable range is 24μH - 1.2 mH, and it is suitable for operating frequencies ranging from DC to 200MHz. It is a compact component that can be easily installed, powered and adjusted.
The WVL9FJ103K adjustable inductor is widely employed in RF circuits due to its strong performance, dynamic range, and ease of adjustment. It is typically used to adjust impedance, match bandgap characteristics, and achieve wide bandwidth with low distortion when implemented in RF circuits. Furthermore, it can also be used in energy harvesting, power management systems, and automotive applications.
The working principle of the WVL9FJ103K adjustable inductor can be explained in terms of the Faraday\'s law of induction. According to this law, a voltage is induced in a conducting element when a magnetic field is changed with respect to time. When current passes through a core of the inductor, a magnetic field is generated around it. This, in turn, creates a voltage across the inductor, which is proportional to the rate at which the current changes. Thus, by adjusting the inductance value, the magnetic field is changed, thus creating a voltage.
In order to achieve higher quality inductors, the WVL9FJ103K employs a metallized polyester construction. This structure ensures that the inductor is strong and reliable. Furthermore, the metallized surface technology also helps in preventing the inductor from vibrating or getting damaged due to external vibrations or shocks. This ensures that the inductor remains stable during operation, thus improving its performance.
In conclusion, the WVL9FJ103K is an adjustable inductor of great performance and durability. It is widely employed in RF circuits due to its adjustable range, compact dimensions and ability to adjust impedance, match bandgap characteristics and achieve high bandwidth with low distortion. The working principle of the device is based on Faraday\'s law of induction and employs a metallized polyester construction, making it reliable and durable.
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Part Number | Manufacturer | Price | Quantity | Description |
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WVL9EB120K | Vishay Dale | 0.0 $ | 1000 | WVL 12 10% EB E212H Adjus... |
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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