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
  
                         
NLCV32T-R15M-EFR


RF Inductors - SMD 150nH 28.8mohms 2.6A 125C Wound Ferrite
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TDK 4543
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.1413

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Wirewound1210 (3225 METRIC)Unshielded150 nH20 %2.6 A28.8 mOhms-- 40 C+ 125 C10500 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFRReel , Cut Tape
1210ASM-1R0J-01


RF Inductors - SMD RF CHIP INDUCTORS NON-MAGNETIC
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Fastron 776
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.4843

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Wirewound1210 (3225 METRIC)Unshielded1 uH5 %330 mA2.16 Ohms-- 40 C+ 150 C35290 MHzStandard3.8 mm3 mm2.4 mm-CeramicAEC - Q2001210ASMReel , Cut Tape
LBM2016T820J


RF Inductors - SMD 963-LSQMB201616T820J RPLCMT PN 0806 82uH 10.01Ohms 5% 85mA
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Taiyo Yuden 773
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AUD 0.0983

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Wirewound0806 (2016 METRIC)Unshielded82 uH5 %85 mA10.01 Ohms-- 40 C+ 105 C2010 MHzStandard2 mm1.6 mm1.8 mm-  LBMReel , Cut Tape
LQW15AN40NJ00D


RF Inductors - SMD
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Murata 771
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.0741

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Wirewound0402 (1005 METRIC)Unshielded40 nH5 %250 mA700 mOhms-- 55 C+ 125 C253 GHzStandard1 mm0.5 mm0.5 mm-  LQWReel , Cut Tape
LQW18AN6N2C8ZD


RF Inductors - SMD 6.2 UH .2%
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Murata 762
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.1483

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 0603 (1608 METRIC) 6.2 nH 1.9 A40 mOhms - 55 C+ 125 C406.65 GHz 1.65 mm0.99 mm0.9 mm   LQW18AN_8ZReel , Cut Tape
LQW43FT180M0HL


RF Inductors - SMD 18 UH 20%
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Murata 755
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 2.1721

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 010 (4532 METRIC) 18 uH 845 mA160 mOhms - 40 C+ 125 C   4.5 mm3.2 mm3.5 mm   LQW43FT_0HReel , Cut Tape
LQW21HN1R2J00L


RF Inductors - SMD
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Murata 747
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.2914

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
LQW15AN8N3C1ZD


RF Inductors - SMD
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 746
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.1474

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded8.3 nH0.2 nH640 mA79 mOhms-- 55 C+ 125 C307.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
0402F-R27K-08


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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Fastron 746
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.4968

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded270 nH10 %380 mA550 mOhms-- 40 C+ 85 C-880 MHzStandard1 mm0.5 mm0.7 mm-FerriteAEC - Q2000402FReel , Cut Tape
MLF1005GR47JT000


470 nH Shielded Multilayer Inductor 50 mA 420mOhm Max 0402 (1005 Metric)
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TDK 658
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.1552

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Multilayer0402 (1005 METRIC)Shielded470 nH5 %50 mA420 mOhms-- 55 C+ 125 C30460 MHzStandard1 mm0.5 mm0.5 mm-Ferrite MLFReel , Cut Tape
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