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
  
                         
B82422A3471K100


RF Inductors - SMD 470nH 150mA 10% 1210 SMD, AEC-Q200
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TDK 5801
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3124

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded470 nH10 %150 mA2.2 Ohms-- 55 C+ 145 C22480 MHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422AReel , Cut Tape
LQW18AN7N5D00D


RF Inductors - SMD 7.5 NH +-.5NH
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Murata 5798
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0806

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded7.5 nH0.5 nH750 mA82 mOhms-- 55 C+ 125 C356 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQP03HQ0N8B02D


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 5797
Ships to you
between Fri. 21 Nov to Thu. 27 Nov
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AUD 0.0448

Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded800 pH0.1 nH1.1 A40 mOhms-- 55 C+ 125 C2018 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
PE-1008CLH1R0STS


RF Inductors - SMD 1008 1uH 1600mA DCR=78mOhms RF
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Pulse 5795
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2868

Multiples of: 1

Multilayer1008 (2520 METRIC)Shielded1 uH-1.6 A75 mOhms1.4 A- 40 C+ 85 C-70 MHzStandard2.5 mm2 mm1 mm-Ceramic PE - 1008CLHReel , Cut Tape
NLV32T-181J-EFD


RF Inductors - SMD 180uH 17ohms 60mA Wound Fer AEC-Q200
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TDK 5793
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.163

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Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded180 uH5 %60 mA17 Ohms-- 40 C+ 105 C207 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
LQH2HNH3R9J03L


RF Inductors - SMD 3.9uH 250mA 5% PWRTRN AEC-Q200
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Murata 5790
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3008

Multiples of: 1

Wirewound2.5 mm x 2 mm x 0.5 mmUnshielded3.9 uH5 % 425 mOhms - 40 C+ 125 C 75 MHzStandard2.5 mm2 mm0.9 mm  AEC - Q200LQH2HNH_03Reel , Cut Tape
LQG15HH5N6C02D


RF Inductors - SMD
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Murata 5786
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1131

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded5.6 nH0.2 nH650 mA180 mOhms-- 55 C+ 125 C84.5 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
IMC0603ER33NJ01


RF Inductors - SMD .033uh 5%
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Vishay 5786
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1676

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Wirewound0603 (1608 METRIC) 33 nH  15 mOhms - 40 C+ 125 C  Standard1.6 mm1.05 mm1.05 mm Ceramic IMCReel , Cut Tape
IMC0603ER56NJ01


RF Inductors - SMD 56nH 5%
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Vishay 5776
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1696

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded56 nH5 %600 mA310 mOhms-- 40 C+ 125 C401.9 GHzStandard1.6 mm1.05 mm1.05 mm-Ceramic IMCReel , Cut Tape
LQG18HN1N2S00D


RF Inductors - SMD 1.2 NH +-.3NH
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Murata 5752
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.054

Multiples of: 10

Multilayer0603 (1608 METRIC)Unshielded1.2 nH0.3 nH1.1 A100 mOhms-- 40 C+ 85 C126 GHzStandard1.6 mm0.8 mm0.8 mm-Air LQGReel , Cut Tape
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