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
  
                         
B82422T1331J000


RF Inductors - SMD SMT-INDUCTOR 1210 0.33UH 5%, AEC-Q200
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TDK 5219
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3635

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Wirewound1210 (3225 METRIC)Unshielded330 nH5 %450 mA230 mOhms-- 55 C+ 125 C30500 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422TReel , Cut Tape
LQG15HZ5N1S02D


RF Inductors - SMD
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Murata 5210
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AUD 0.0505

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Multilayer0402 (1005 METRIC)Unshielded5.1 nH0.3 nH650 mA180 mOhms-- 55 C+ 125 C85.3 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQW2BAS91NG00L


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 5210
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1393

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Wirewound0805 (2015 METRIC)Unshielded91 nH2 %400 mA480 mOhms-- 55 C+ 125 C651.33 GHzStandard2.09 mm1.53 mm1.42 mm-  LQW2BAReel , Cut Tape
LBM2016T1R0J


RF Inductors - SMD 963-LSQMB201616T1R0J RPLCMT PN 0806 1uH 494mOhms 5% 385mA
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Taiyo Yuden 5200
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AUD 0.0855

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Wirewound0806 (2016 METRIC)Unshielded1 uH5 %385 mA494 mOhms-- 40 C+ 105 C30220 MHzStandard2 mm1.6 mm1.8 mm-  LBMReel , Cut Tape
LQW18AN47NG80D


RF Inductors - SMD 47 NH 2% NH
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Murata 5195
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AUD 0.1004

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Wirewound0603 (1608 METRIC)Unshielded47 nH2 %830 mA230 mOhms-- 55 C+ 125 C322.7 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
MLG1005S2N4STD25


RF Inductors - SMD IND 0402 2.4nH StdQ AEC Q200 RF IND
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TDK 5189
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AUD 0.0225

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Multilayer0402 (1005 METRIC)Unshielded2.4 nH0.3 nH800 mA150 mOhms-- 55 C+ 125 C78.2 GHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
MHL1ECTTP3N3S


RF Inductors - SMD 3.3nH +/-0.3nH
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KOA Speer 5188
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AUD 0.1082

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Multilayer0402 (1005 METRIC)Unshielded3.3 nH0.3 nH150 mA220 mOhms-- 55 C+ 125 C87 GHzStandard1 mm0.5 mm0.5 mm-Ceramic MHLReel , Cut Tape
LQW18AS8N2G0ZD


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 5188
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1293

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Wirewound0603 (1608 METRIC)Unshielded8.2 nH2 %700 mA115 mOhms-- 40 C+ 125 C304.2 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQG18HH2N7S00D


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 5188
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1319

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Multilayer0603 (1608 METRIC)Unshielded2.7 nH0.3 nH1 A130 mOhms-- 55 C+ 125 C124 GHzStandard1.6 mm0.8 mm0.8 mm-AirAEC - Q200LQGReel , Cut Tape
CW201212-33NJ


Inductor RF Wirewound 0.033uH 5% 250MHz 60Q-Factor Ceramic 0.5A 0.27Ohm DCR 0805 T/R
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Bourns 5127
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AUD 0.1944

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Wirewound0805 (2012 METRIC)Unshielded33 nH5 %500 mA150 mOhms-- 40 C+ 125 C602.4 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW201212Reel , Cut Tape
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