RF inductors - SMD

RF (Radio Frequency) inductors in SMD (Surface Mount Device) form are specialized components used in high-frequency electronic circuits and applications. SMD RF inductors are designed to be mounted directly onto the surface of a circuit board, offering advantages such as space-saving, easy assembly, and compatibility with automated manufacturing processes.
RF inductors are specifically optimized for operation at radio frequency ranges, typically from a few megahertz (MHz) up to several gigahertz (GHz). They are commonly used in RF applications, including RF filters, oscillators, RF amplifiers, impedance matching networks, and wireless communication systems.
SMD RF inductors feature a compact design and are constructed similarly to other inductors. They consist of a coil wound on a core material, but with specific considerations for high-frequency performance and minimizing parasitic effects. These parasitic effects include self-capacitance, series resistance, and interwinding capacitance, which can impact the inductor's performance at high frequencies.
The core materials used in SMD RF inductors are carefully chosen to provide high magnetic permeability, low losses, and stable performance across the desired frequency range. Common core materials for RF inductors include ceramic materials, ferrite, and powdered iron.
SMD RF inductors come in various package sizes and shapes, denoted by standardized codes such as 0402, 0603, or 0805, indicating their dimensions in terms of length and width. This allows for easy integration into surface mount technology and efficient assembly onto circuit boards.
When selecting SMD RF inductors, critical parameters to consider include inductance value, quality factor (Q factor), self-resonant frequency (SRF), and maximum current handling capability. The inductance value determines the component's ability to store energy in its magnetic field, while the Q factor represents its efficiency and ability to maintain high-quality performance. The SRF indicates the frequency at which the inductor starts to exhibit resonance due to its parasitic capacitance. Maximum current handling capability is crucial for ensuring the inductor can withstand the power demands of the RF circuit.
SMD RF inductors are chosen based on specific circuit requirements, such as the desired operating frequency, impedance matching, bandwidth, and available board space. They are essential components in RF systems, contributing to impedance control, filtering, and energy storage functions necessary for reliable and efficient RF signal processing and wireless communication.

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Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
LQW18AN13NJ00D


RF Inductors - SMD 13 NH 5%
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Murata 1965
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between Mon. 20 Jul to Wed. 22 Jul
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AUD 0.0827

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded13 nH5 %600 mA130 mOhms-- 55 C+ 125 C356 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
CW252016-82NJ


RF Inductors - SMD 82 NH 5% WIREWOUND
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Bourns 1475
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between Mon. 20 Jul to Wed. 22 Jul
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AUD 0.2052

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded82 nH5 %600 mA180 mOhms-- 40 C+ 125 C601 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
LQW2UAS68NF00L


RF Inductors - SMD 68 NH 1%
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Murata 1468
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between Mon. 20 Jul to Wed. 22 Jul
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AUD 0.2879

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Wirewound1008 (2520 METRIC)Unshielded68 nH1 %1 A200 mOhms-- 55 C+ 125 C651.3 GHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
CW252016-4R7J


RF Inductors - SMD 4.7 UH 5%
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Bourns 1460
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between Mon. 20 Jul to Wed. 22 Jul
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AUD 0.181

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Wirewound1008 (2520 METRIC)Unshielded4.7 uH5 %175 mA2.3 Ohms-- 40 C+ 125 C1843 MHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
AS0713N7GTR


RF Inductors - SMD 13.7nH 2% SQUARE AIR CORE
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Kyocera AVX 1456
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between Mon. 20 Jul to Wed. 22 Jul
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AUD 0.4423

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Wirewound1.829 mm x 1.524 mm x 1.93 mmUnshielded13.7 nH2 %2.7 A8 mOhms-- 40 C+ 125 C1004.3 GHzStandard1.93 mm1.829 mm1.524 mm-Air ASReel , Cut Tape
MLF2012K470M


RF Inductors - SMD 47uH
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TDK 1455
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between Mon. 20 Jul to Wed. 22 Jul
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AUD 0.101

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Multilayer0805 (2012 METRIC)Shielded47 uH20 %4 mA2.7 Ohms-- 55 C+ 125 C3520 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
PM1210-3R3J-RC


Ind Chip Molded Bobbin Core 3.3uH 5% 7.96MHz 30Q-Factor Ferrite 180mA 1210 T/R
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Bourns 1455
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between Tue. 14 Jul to Mon. 20 Jul
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AUD 0.2729

Multiples of: 2000

Wirewound1210 (3225 METRIC)Unshielded3.3 uH5 %260 mA1.2 Ohms-- 55 C+ 105 C3060 MHzStandard2.9 mm2.5 mm2.2 mm-Ferrite PM1210Reel , Cut Tape
PM1008-R10K-RC


RF Inductors - SMD 0.10uH 10%
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Bourns 1455
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between Mon. 20 Jul to Wed. 22 Jul
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AUD 0.2868

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded100 nH10 %650 mA560 mOhms-- 55 C+ 125 C601 GHzStandard2.5 mm2 mm1.6 mm-Ceramic PM1008Reel , Cut Tape
PM105SB-221K-RC


Inductor Power Shielded Bobbin Core 220uH 10% 100KHz 27Q-Factor Ferrite 470mA 780mOhm DCR T/R
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Bourns 1455
Ships to you
between Tue. 14 Jul to Mon. 20 Jul
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AUD 0.7836

Multiples of: 1

Wirewound Shielded220 uH20 %470 mA780 mOhms-- 30 C+ 100 C275 MHzStandard4.5 mm--9.9 mmFerrite PM105SBReel , Cut Tape
LQW15AN3N9C80D


Ind RF Chip Unshielded Wirewound 3.9nH 0.2nH 100MHz 35Q-Factor Air 1.95A 0402 Paper T/R
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Murata 1448
Ships to you
between Mon. 20 Jul to Wed. 22 Jul
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AUD 0.1051

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded3.9 nH0.2 nH1.95 A30 mOhms-- 55 C+ 125 C3510 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
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