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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(Ex. GST)(▲▼)		Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
LQW15AN8N8G80D


RF Inductors - SMD
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Murata 9680
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AUD 0.1283
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Wirewound0402 (1005 METRIC)Unshielded8.8 nH2 %1.42 A70 mOhms-- 55 C+ 125 C316.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQW15AN3N0D80D


RF Inductors - SMD
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Murata 9680
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AUD 0.1312
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Wirewound0402 (1005 METRIC)Unshielded3 nH0.5 nH1.35 A63 mOhms - 55 C+ 125 C2012.5 GHzStandard1 mm0.6 mm0.6 mm   LQWReel , Cut Tape
LQG15WH2N4B02D


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 9680
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AUD 0.1376
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Multilayer0402 (1005 METRIC)Unshielded2.4 nH0.1 nH1 A60 mOhms-- 55 C+ 125 C236.5 GHzStandard1 mm0.6 mm0.5 mm-Air LQGReel , Cut Tape
LQW15AN2N3C1ZD


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 9680
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AUD 0.1474
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Wirewound0402 (1005 METRIC)Unshielded2.3 nH0.2 nH1 A27 mOhms-- 55 C+ 125 C2514 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LQG15WZ3N6B02D


RF Inductors - SMD
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Murata 9680
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AUD 0.1485
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Multilayer0402 (1005 METRIC)Unshielded3.6 nH0.1 nH900 mA90 mOhms-- 55 C+ 125 C235.5 GHzStandard1 mm0.6 mm0.5 mm-Air LQGReel , Cut Tape
IWC0805DR10R-3G


RF Inductors - SMD 0805 100nH 2% 400mA
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Laird Performance Materials 9680
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AUD 0.1606
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Wirewound2.35 mm x 1.73 mm x 1.52 mmUnshielded100 nH2 %400 mA460 mOhms-- 40 C+ 125 C651.2 GHzStandard2.35 mm1.73 mm1.52 mm-Ceramic IWC0805Reel , Cut Tape
IWC1008DR82R-3G


RF Inductors - SMD 1008 820nH 2% 400mA
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Laird Performance Materials 9680
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AUD 0.2095
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Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded820 nH2 %400 mA1.62 Ohms-- 40 C+ 125 C45350 MHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
LBM2016T5R6J


RF Inductors - SMD 963-LSQMB201616T5R6J RPLCMT PN 0806 5.6uH 1144mOhms 5% 255mA
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Taiyo Yuden 9677
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AUD 0.0843
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Wirewound0806 (2016 METRIC)Unshielded5.6 uH5 %255 mA1.14 Ohms-- 40 C+ 105 C2536 MHzStandard2 mm1.6 mm1.8 mm-  LBMReel , Cut Tape
LQG15WZ3N1B02D


RF Inductors - SMD Fixed IND 3.1nH 900mA INFOTMT
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Murata 9675
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AUD 0.1319
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Multilayer0402 (1005 METRIC)Unshielded3.1 nH0.1 nH900 mA90 mOhms-- 55 C+ 125 C236 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQW15AN3N0G8ZD


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 9675
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AUD 0.1415
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Wirewound0402 (1005 METRIC)Unshielded3 nH2 %1.35 A63 mOhms-- 55 C+ 125 C2012.5 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
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