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
  
                         
CWF1610-4R7K


RF Inductors - SMD Ind,1.6x1x1mm,4.7uH+/-10%,0.42A,non-shd
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Bourns 7695
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between Wed. 26 Nov to Fri. 28 Nov
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AUD 0.0891

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Wirewound0603 (1610 METRIC)Semi - Shielded4.7 uH10 %420 mA -- 40 C+ 125 C--Standard1.6 mm1 mm1 mm-Ferrite CWF1610Reel , Cut Tape
MHQ1005PR51GT000


RF Inductors - SMD IND 0402 510nH S-HQ SMD RF IND
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TDK 7694
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AUD 0.0909

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Multilayer0402 (1005 METRIC)Unshielded510 nH2 %70 mA10.2 Ohms-- 55 C+ 125 C13520 MHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
LQW15AN8N0C1ZD


RF Inductors - SMD
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Murata 7694
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between Wed. 26 Nov to Fri. 28 Nov
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AUD 0.1352

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Wirewound0402 (1005 METRIC)Unshielded8 nH0.2 nH640 mA79 mOhms-- 55 C+ 125 C307.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
WCLA3225V1-6R8-R


RF Inductors - SMD Chip IND 6.8uH 0.66A SMT 2 Pad
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Eaton 7690
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AUD 0.2706

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Wirewound1210 (3225 METRIC)Shielded6.8 uH10 %660 mA300 mOhms - 55 C+ 125 C1034 MHz 3.6 mm2.8 mm2.4 mm Ferrite WCLAReel , Cut Tape
LQG15HSR10H02D


RF Inductors - SMD
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Murata 7687
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between Wed. 26 Nov to Fri. 28 Nov
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AUD 0.0391

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Multilayer0402 (1005 METRIC)Unshielded100 nH3 %200 mA1.25 Ohms-- 55 C+ 125 C8600 MHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQW2BAS43NJ00L


43 nH Unshielded Wirewound Inductor 500 mA 340mOhm Max 0805 (2015 Metric)
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Murata 7685
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AUD 0.124

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Wirewound0805 (2015 METRIC)Unshielded43 nH5 %500 mA340 mOhms-- 55 C+ 125 C601.8 GHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
B82498F3331J001


RF Inductors - SMD SMT-INDUCTOR 0805 330 NH 5%
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TDK 7678
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between Wed. 26 Nov to Fri. 28 Nov
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AUD 0.3622

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Wirewound0805 (2012 METRIC)Unshielded330 nH5 %220 mA1.5 Ohms-- 55 C+ 125 C45800 MHzStandard2 mm1.3 mm1.4 mm-CeramicAEC - Q200B82498FReel , Cut Tape
MLG1005S1N6CT000


RF Inductors - SMD IND 0402 1.6nH StdQ SMD RF IND
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TDK 7677
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AUD 0.0727

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Multilayer0402 (1005 METRIC)Unshielded1.6 nH0.2 nH1 A120 mOhms-- 55 C+ 125 C79.4 GHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , Cut Tape
MLG1005SR39JTD25


RF Inductors - SMD IND 0402 390nH StdQ AEC Q200 RF IND
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TDK 7677
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AUD 0.0847

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Multilayer0402 (1005 METRIC)Unshielded390 nH5 %50 mA8 Ohms-- 55 C+ 125 C6400 MHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
LQW15AN9N5G80D


RF Inductors - SMD
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Murata 7668
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between Wed. 26 Nov to Fri. 28 Nov
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AUD 0.1514

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Wirewound0402 (1005 METRIC)Unshielded9.5 nH2 %1.4 A81 mOhms-- 55 C+ 125 C326 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
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