Allicdata Part #: | WVL9FJ2R7KH-ND |
Manufacturer Part#: |
WVL9FJ2R7KH |
Price: | $ 0.00 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | WVL-H 2.7 10% F09 |
More Detail: | 2.7µH Adjustable Inductor 88 @ 7.9MHz Radial, Hori... |
DataSheet: | WVL9FJ2R7KH Datasheet/PDF |
Quantity: | 1000 |
1 +: | 0.00000 |
Series: | WVL |
Part Status: | Obsolete |
Inductance: | 2.7µH |
Tolerance: | ±10% |
Q @ Freq: | 88 @ 7.9MHz |
Mounting Type: | Through Hole |
Package / Case: | Radial, Horizontal Cylinder |
Size / Dimension: | 0.320" Dia x 0.400" L (8.13mm x 10.16mm) |
Height: | -- |
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Adjustable inductors have long been seen as prime components in many various electrical circuits. This is due to the fact that they offer a wide variety of adjustable parameters for inductance, allowing for precise control of the electrical circuits they are used in. One such adjustable inductor is the WVL9FJ2R7KH. In this article we will discuss the application field and working principle of the WVL9FJ2R7KH.
Applications of the WVL9FJ2R7KH
The WVL9FJ2R7KH adjustable inductor is widely used in communication and conversion circuits. It is used for the impedance matching of the amplifier, the coupling and decoupling of the oscillator, the re-sampling of the digital data, the elimination of the interference, the resonance of the oscillator, and the auto-tuning of the voltage-controlled oscillator. This inductor is also used in switching power supplies, HF and RF communications, and in the miniaturization of electrical circuits.
Working Principle of the WVL9FJ2R7KH
The WVL9FJ2R7KH is an adjustable inductor that is composed of five components: an inductance coil, two capacitors, and two resistors. The two capacitors are connected in parallel to one another and to the inductance coil. The inductance coil is also connected to the two resistors, each in series to one another. The resistor on the left is adjustable to vary the inductance value. This is done by adjusting the resistance in the circuit, which in turn alters the inductance of the coil.
The inductance of the coil is dependent on the values of the capacitance and resistance in the circuit, as well as the core material of the coil. The core material used for the WVL9FJ2R7KH affects the inertia of the coil and, consequently, the inductance value. For these reasons, the WVL9FJ2R7KH adjustable inductors have a wide range of application uses, as they offer a high degree of adjustability.
Conclusion
The WVL9FJ2R7KH adjustable inductor is a versatile component that is widely used in communication and conversion circuits. This versatile inductor offers a wide range of adjustable parameters for inductance, making it ideal for those who need precise control of the electrical circuits they are used in. Thanks to its five components – an inductance coil, two capacitors, and two resistors – the WVL9FJ2R7KH adjustable inductor is able to offer a wide range of application uses, from switching power supplies to HF and RF communications.
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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