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
  
                         
LQW18AN5N6C80D


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 6707
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.1019

Multiples of: 5

Wirewound0603 (1608 METRIC)Unshielded5.6 nH0.2 nH1.9 A40 mOhms-- 55 C+ 125 C386.65 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
LQW18AS3N3G00D


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 3889
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0702

Multiples of: 10

Wirewound0603 (1608 METRIC)Unshielded3.3 nH2 %700 mA45 mOhms-- 40 C+ 125 C355.9 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
L02012R7BHSTR


RF Inductors - SMD 2.7nH
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Kyocera AVX 3841
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2475

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Thin Film0201 (0603 METRIC)Unshielded2.7 nH0.1 nH180 mA700 mOhms-- 55 C+ 125 C714 GHzStandard0.6 mm0.325 mm0.225 mm   Accu - LReel , Cut Tape
MLF2012DR68KTD25


RF Inductors - SMD 680nH 600mohms 150mA +/-10% Fer AEC-Q200
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TDK 3840
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1438

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Multilayer0805 (2012 METRIC)Shielded680 nH10 %150 mA600 mOhms-- 55 C+ 125 C25190 MHzStandard2 mm1.25 mm1.25 mm-FerriteAEC - Q200MLFReel , Cut Tape
AISC-Q0402HQ-15NG-T


RF Inductors - SMD IND 15nH 1.1A 110m?
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Abracon 3839
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AUD 0.1981

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Wirewound0402 (1208 METRIC)Unshielded15 nH2 %1.1 A110 mOhms - 40 C+ 125 C853.9 GHzStandard1.27 mm0.76 mm0.61 mm Ceramic AISC - Q0402HQReel , Cut Tape
ILSB0603ER3R9K


RF Inductors - SMD 3.9uH 10%
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Vishay 3837
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AUD 0.0852

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Established Reliability0603 (1608 METRIC)Shielded3.9 uH10 %15 mA1.7 Ohms-- 55 C+ 125 C3541 MHzStandard1.6 mm0.8 mm0.8 mm-  ILSB - 0603Reel , Cut Tape
LQW15AN24NG0ZD


RF Inductors - SMD
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Murata 3836
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1252

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded24 nH2 %280 mA520 mOhms-- 55 C+ 125 C253.5 GHzStandard1 mm0.5 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
MCLA2012V1-R820-R


RF Inductors - SMD MCLA Auto Chip IND 2012 0.82uH 2 Pads
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Eaton 3831
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0637

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   820 nH10 %             AEC - Q200MCLAReel , Cut Tape
IMC0805ER39NJ01


RF Inductors - SMD .039uh 5%
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Vishay 3831
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1848

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded39 nH  180 mOhms - 40 C+ 125 C 2.1 GHzStandard2 mm1.25 mm1.2 mm Ceramic IMCReel , Cut Tape
LQW18AN6N8C80D


RF Inductors - SMD
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Murata 3787
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0883

Multiples of: 5

Wirewound0603 (1608 METRIC)Unshielded6.8 nH0.2 nH1.9 A40 mOhms-- 55 C+ 125 C406.65 GHzStandard1.65 mm0.99 mm0.9 mm-- LQWReel , Cut Tape
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