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
  
                         
LCWC0603J22NGTAR


RF Inductors - SMD 22nH 0603 5%
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Kyocera AVX 3864
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AUD 0.1284

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Wirewound0603 (1608 METRIC)Unshielded22 nH5 %700 mA190 mOhms-- 40 C+ 125 C383 GHzStandard1.8 mm1.02 mm1.12 mm Ceramic LCWCReel , Cut Tape
NLV25T-2R7J-EFD


RF Inductors - SMD 2.7uH 1.7ohms 195mA Wound Fer AEC-Q200
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TDK 3864
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.184

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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded2.7 uH5 %195 mA1.7 Ohms-- 40 C+ 105 C3070 MHzStandard2.5 mm2 mm1.8 mm-FerriteAEC - Q200NLV25 - EFDReel , Cut Tape
LQW18AN51NG0ZD


RF Inductors - SMD
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Murata 3863
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1222

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Wirewound0603 (1608 METRIC)Unshielded51 nH2 %370 mA330 mOhms-- 55 C+ 125 C382.5 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQW18AN51NJ80D


RF Inductors - SMD
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Murata 3862
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1065

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Wirewound0603 (1608 METRIC)Unshielded51 nH5 %830 mA230 mOhms - 55 C+ 125 C322.7 GHzStandard1.65 mm0.99 mm0.9 mm   LQWReel , Cut Tape
MLF2012A3R9KTD25


RF Inductors - SMD 3.9uH 650mohms 30mA +/-10% Fer AEC-Q200
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TDK 3861
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AUD 0.2205

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Multilayer0805 (2012 METRIC)Shielded3.9 uH10 %30 mA650 mOhms-- 55 C+ 125 C4580 MHzStandard2 mm1.25 mm1.25 mm-FerriteAEC - Q200MLFReel , Cut Tape
AISC-0603-R0051J-T


RF Inductors - SMD FIXED IND 5.1NH 600MA 130 MOHM
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ABRACON 3860
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AUD 0.1558

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Wirewound0603 (1812 METRIC)Unshielded5.1 nH5 %600 mA130 mOhms - 40 C+ 125 C216 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - 0603Reel , Cut Tape
AISC-Q0402HQ-2N2C-T


RF Inductors - SMD IND 2.2nH 2.1A 38m?
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Abracon 3860
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AUD 0.2133

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Wirewound0402 (1208 METRIC)Unshielded2.2 nH0.2 nH2.1 A38 mOhms - 40 C+ 125 C8615.1 GHzStandard1.27 mm0.76 mm0.61 mm Ceramic AISC - Q0402HQReel , Cut Tape
0603AQC-R39J-01


RF Inductors - SMD Wire-wound Ceramic Chip Inductor AEC-200
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Fastron 3860
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AUD 0.2438

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Chip Inductor0603 (1608 METRIC)Unshielded390 nH5 %250 mA2.1 Ohms - 40 C+ 140 C27650 MHzStandard1.7 mm1.12 mm1.05 mm CeramicAEC - Q200 Reel , Cut Tape
B82422A1562K100


RF Inductors - SMD SMT-INDUCTOR 1210 5.6 UH 10%, AEC-Q200
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TDK 3860
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3086

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Wirewound1210 (3225 METRIC)Unshielded5.6 uH10 %140 mA2.6 Ohms-- 55 C+ 145 C27100 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
LQW15AN9N0J80D


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 3858
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1096

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded9 nH5 %1.42 A70 mOhms-- 55 C+ 125 C306.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
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