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
  
                         
S1210R-182K


RF Inductors - SMD 1.8uH 10%
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API Delevan 930
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AUD 2.9885
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Wirewound1210 (3225 METRIC)Shielded1.8 uH10 %498 mA650 mOhms-- 55 C+ 125 C4095 MHzStandard3.51 mm2.66 mm2.57 mm-Ferrite S1210/RReel , Cut Tape
MHQ1005075HA4N2STD25


RF Inductors - SMD FIXED IND 4.2NH 0.65A 120 MOHM SMD
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TDK 926
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AUD 0.11
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Multilayer Ceramic Inductor0402 (1005 METRIC)Shielded4.2 nH0.3 nH650 mA120 mOhms - 55 C+ 125 C207.4 GHzStandard1 mm0.5 mm0.7 mm Ceramic MHQReel , Cut Tape
LQW18AN5N6C0ZD


RF Inductors - SMD
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Murata 926
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AUD 0.1224
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Wirewound0603 (1608 METRIC)Unshielded5.6 nH0.2 nH750 mA82 mOhms-- 55 C+ 125 C356 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQW18AS3N6G0ZD


RF Inductors - SMD 3.6 NH 2%
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Murata 926
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AUD 0.1293
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Wirewound0603 (1608 METRIC)Unshielded3.6 nH2 %700 mA63 mOhms-- 40 C+ 125 C225.9 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQP02HQ22NH02E


RF Inductors - SMD
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Murata 921
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AUD 0.0931
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Thin Film01005 (0402 METRIC)Unshielded22 nH3 %140 mA2.26 Ohms-- 55 C+ 125 C143 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , Cut Tape
MHQ1005075HA3N2STD25


RF Inductors - SMD FIXED IND 3.2NH 0.8A 90 MOHM SMD
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TDK 921
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AUD 0.11
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Multilayer Ceramic Inductor0402 (1005 METRIC)Shielded3.2 nH0.3 nH800 mA90 mOhms - 55 C+ 125 C209.7 GHzStandard1 mm0.5 mm0.7 mm Ceramic MHQReel , Cut Tape
IMC1008ERR47J


RF Inductors - SMD 470nH 5%
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Vishay 921
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AUD 0.1958
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Wirewound1008 (2520 METRIC)Unshielded470 nH5 %420 mA1.17 Ohms-- 40 C+ 125 C45480 MHzStandard2.5 mm2 mm1.6 mm-Ceramic IMCReel , Cut Tape
WCLA1608V1-1R6-R


RF Inductors - SMD 1.6 NH 10% AEC-Q200
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Eaton 921
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AUD 0.206
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Wirewound0603 (1608 METRIC)Unshielded1.6 nH10 %700 mA40 mOhms-- 40 C+ 125 C1812.5 GHzStandard1.78 mm1.1 mm0.95 mm- AEC - Q200WCLAReel , Cut Tape
AS0710N2GTR


RF Inductors - SMD 10.2nH 2% SQUARE AIR CORE
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Kyocera AVX 920
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AUD 0.3987
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Wirewound1.829 mm x 1.524 mm x 1.626 mmUnshielded10.2 nH2 %2.7 A7 mOhms-- 40 C+ 125 C1004 GHzStandard1.626 mm1.829 mm1.524 mm-Air ASReel , Cut Tape
L08058R2DEWTR


RF Inductors - SMD 8.2nH
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Kyocera AVX 919
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AUD 0.9464
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Thin Film0805 (2012 METRIC)Unshielded8.2 nH0.5 nH1.5 A120 mOhms-- 55 C+ 125 C433.5 GHzStandard2.11 mm1.5 mm0.91 mm-  0603, 0805Reel , Cut Tape
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