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
  
                         
MLG0603S0N5CT000


RF Inductors - SMD IND 0201 0.5nH StdQ SMD RF IND
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TDK 12069
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between Mon. 24 Nov to Wed. 26 Nov
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AUD 0.0441

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded500 pH0.2 nH600 mA100 mOhms-- 55 C+ 125 C-20 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLGReel , Cut Tape
AIML-1206-1R0K-T


RF Inductors - SMD 1 UH +/-10%
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ABRACON 12068
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between Tue. 18 Nov to Mon. 24 Nov
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AUD 0.1694

Multiples of: 1

Multilayer Ferrite Chip Inductor1206 (3216 METRIC)Shielded1 uH10 %100 mA400 mOhms - 55 C+ 125 C5090 MHzStandard3.2 mm1.6 mm1.1 mm Ferrite AIML - 1206Reel , Cut Tape
LQP03TG3N5B02D


RF Inductors - SMD
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Murata 12014
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between Mon. 24 Nov to Wed. 26 Nov
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AUD 0.022

Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded3.5 nH0.1 nH350 mA350 mOhms - 55 C+ 125 C138 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
MLG0603P1N1CT000


RF Inductors - SMD IND 0201 1.1nH Hi-Q SMD RF IND
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TDK 12014
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between Mon. 24 Nov to Wed. 26 Nov
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AUD 0.0273

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded1.1 nH0.2 nH1 A70 mOhms-- 55 C+ 125 C1419.9 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
MLG1005SR22JTD25


RF Inductors - SMD IND 0402 220nH StdQ AEC Q200 RF IND
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TDK 12011
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between Mon. 24 Nov to Wed. 26 Nov
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AUD 0.0852

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded220 nH5 %100 mA4.2 Ohms-- 55 C+ 125 C8500 MHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
LQP02HQ2N7B02E


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 11988
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between Mon. 24 Nov to Wed. 26 Nov
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AUD 0.107

Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded2.7 nH0.1 nH450 mA200 mOhms-- 55 C+ 125 C148.8 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQW15AN13NJ80D


RF Inductors - SMD
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Murata 11984
Ships to you
between Mon. 24 Nov to Wed. 26 Nov
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AUD 0.1312

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded13 nH5 %1.24 A93 mOhms-- 55 C+ 125 C305 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQW15AN2N3G8ZD


RF Inductors - SMD 2.3 NH
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Murata 11946
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between Mon. 24 Nov to Wed. 26 Nov
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AUD 0.119

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded2.3 nH2 %2.53 A22 mOhms-- 55 C+ 125 C3015.5 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQW18ANR10J80D


RF Inductors - SMD
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Murata 11941
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between Mon. 24 Nov to Wed. 26 Nov
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AUD 0.1079

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded100 nH5 %490 mA630 mOhms-- 55 C+ 125 C341.75 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
B82422A1103J100


RF Inductors - SMD SMT-INDUCTOR 1210 10 UH 5%, AEC-Q200
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TDK 11936
Ships to you
between Mon. 24 Nov to Wed. 26 Nov
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AUD 0.319

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded10 uH5 %180 mA1.6 Ohms-- 55 C+ 145 C2725 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
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