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
  
                         
AISC-Q0402HQ-3N9C-T


RF Inductors - SMD IND 3.9nH 1.7A 45m?
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Abracon 3831
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2133

Multiples of: 1

Wirewound0402 (1208 METRIC)Unshielded3.9 nH0.2 nH1.7 A45 mOhms - 40 C+ 125 C989.5 GHzStandard1.27 mm0.76 mm0.61 mm Ceramic AISC - Q0402HQReel , Cut Tape
AL05B08N8GTR


RF Inductors - SMD 8.8nH 2% AIR CORE
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Kyocera AVX 3831
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.5866

Multiples of: 1

Wirewound1.42 mm x 1.37 mm x 4.04 mmUnshielded8.8 nH2 %1.6 A12 mOhms-- 40 C+ 125 C1006 GHzStandard4.04 mm1.42 mm1.37 mm Air ALReel , Cut Tape
0603AQC-016J-01


RF Inductors - SMD Wire-wound Ceramic Chip Inductor AEC-200
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Fastron 3829
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AUD 0.2438

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Chip Inductor0603 (1608 METRIC)Unshielded16 nH5 %2.5 A70 mOhms - 40 C+ 140 C452.8 GHzStandard1.7 mm1.12 mm1.05 mm CeramicAEC - Q200 Reel , Cut Tape
IMC0805ER12NJ01


RF Inductors - SMD .012uh 5%
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Vishay 3828
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1657

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Wirewound0805 (2012 METRIC)Unshielded12 nH  80 mOhms - 40 C+ 125 C 4.1 GHzStandard2 mm1.25 mm1.2 mm Ceramic IMCReel , Cut Tape
LQW21HN1R2J00L


RF Inductors - SMD
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Murata 3825
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2622

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded1.2 uH5 %100 mA3.12 Ohms-- 40 C+ 85 C35400 MHzStandard2 mm1.2 mm0.9 mm-Ferrite LQWReel , Cut Tape
HL02150GTTR


RF Inductors - SMD 15nH 2%
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Kyocera AVX 3825
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between Fri. 21 Nov to Thu. 27 Nov
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AUD 0.561

Multiples of: 1

Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded15 nH2 %95 mA1.2 Ohms-- 55 C+ 125 C154 GHzStandard1 mm0.58 mm0.35 mm-  HLReel
LQW15AN10NH0ZD


RF Inductors - SMD
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Murata 3822
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1192

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded10 nH3 %500 mA170 mOhms-- 55 C+ 125 C255.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
AIML-0805-R39K-T


RF Inductors - SMD FIXED IND 390NH 200MA 650 MOHM
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ABRACON 3821
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between Fri. 21 Nov to Thu. 27 Nov
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AUD 0.0727

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Multilayer Ferrite Chip Inductor0805 (2012 METRIC)Shielded390 nH10 %200 mA650 mOhms - 55 C+ 125 C25135 MHzStandard2 mm1.25 mm1.25 mm Ferrite AIML - 0805Reel , Cut Tape
ILSB0603ERR10K


RF Inductors - SMD .1uH 10%
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Vishay 3821
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.095

Multiples of: 1

Established Reliability0603 (1608 METRIC)Shielded100 nH10 %50 mA500 mOhms-- 55 C+ 125 C15276 MHzStandard1.6 mm0.8 mm0.8 mm-  ILSB - 0603Reel , Cut Tape
AISC-Q0603HQ-15NG-T


RF Inductors - SMD IND 15nH 1.2A 78m?
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Abracon 3821
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1962

Multiples of: 1

Wirewound0603 (1812 METRIC)Unshielded15 nH2 %1.2 A78 mOhms - 40 C+ 125 C483.6 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - Q0603HQReel , Cut Tape
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