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
  
                         
LQP03TN2N4BZ2D


RF Inductors - SMD
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Murata 15684
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.0398

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Thin Film0201 (0603 METRIC)Unshielded2.4 nH0.1 nH500 mA200 mOhms-- 55 C+ 125 C1410 GHzStandard0.6 mm0.3 mm0.3 mm-FerriteAEC - Q200LQPReel , Cut Tape
LQP03TN11NH02D


RF Inductors - SMD 11 NH 3%
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Murata 15623
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between Fri. 14 Nov to Thu. 20 Nov
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AUD 0.0098

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Thin Film0201 (0603 METRIC)Unshielded11 nH3 %250 mA800 mOhms - 55 C+ 125 C142.9 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
Hot LQP03TNR27H02D


hf inductors 270nh ±3% 60ma 0201 rohs
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Murata 15610
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between Fri. 14 Nov to Thu. 20 Nov
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AUD 0.0156

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Thin Film0201 (0603 METRIC)Unshielded270 nH3 %60 mA15 Ohms - 55 C+ 125 C5450 MHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP02TN2N1B02D


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 15583
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.0485

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Thin Film01005 (0402 METRIC)Unshielded2.1 nH0.1 nH200 mA750 mOhms - 55 C+ 125 C89 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
LQW15AN11NH00D


RF Inductors - SMD
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Murata 15533
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.0785

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Wirewound0402 (1005 METRIC)Unshielded11 nH3 %500 mA140 mOhms-- 55 C+ 125 C305.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
NLV25T-270J-EF


RF Inductors - SMD 27uH 6.3ohms 115mA Wound Ferrite
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TDK 15523
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AUD 0.0412

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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded27 uH5 %115 mA6.3 Ohms-- 40 C+ 105 C2521 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
CI160808-4N7D


RF Inductors - SMD 4.7nH .3% MultiLayer High Frequency
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Bourns 15520
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AUD 0.0455

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Multilayer0603 (1608 METRIC)Unshielded4.7 nH0.3 nH300 mA280 mOhms-- 55 C+ 125 C102.8 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic CI160808Reel , Cut Tape
CS160808-R68K


RF Inductors - SMD 0.68uH '10%
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Bourns 15520
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.077

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Multilayer0603 (1608 METRIC)Shielded680 nH10 %150 mA900 mOhms-- 55 C+ 125 C3080 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite  Reel , Cut Tape
MHQ1005075HA2N2BTD25


RF Inductors - SMD FIXED IND 2.2NH 1A 50 MOHM SMD
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TDK 15520
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.1187

Multiples of: 1

Multilayer Ceramic Inductor0402 (1005 METRIC)Shielded2.2 nH0.1 nH1 A50 mOhms - 55 C+ 125 C2013.1 GHzStandard1 mm0.5 mm0.7 mm Ceramic MHQReel , Cut Tape
LQW15AN2N7G8ZD


RF Inductors - SMD 2.7 NH 2%
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Murata 15517
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.1137

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Wirewound0402 (1005 METRIC)Unshielded2.7 nH2 %1.5 A47 mOhms-- 55 C+ 125 C2814 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
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