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
  
                         
LQW15AN47NJ8ZD


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 9535
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between Tue. 25 Nov to Thu. 27 Nov
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AUD 0.1004

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Wirewound0402 (1005 METRIC)Unshielded47 nH5 %440 mA648 mOhms-- 55 C+ 125 C253.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LQG15HZR10G02D


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 9531
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between Tue. 25 Nov to Thu. 27 Nov
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AUD 0.1232

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Multilayer0402 (1005 METRIC)Unshielded100 nH2 %200 mA1.25 Ohms-- 55 C+ 125 C8600 MHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
NLV25T-220J-EF


RF Inductors - SMD 22uH 5.5ohms 125mA Wound Ferrite
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TDK 9531
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AUD 0.1467

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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded22 uH5 %125 mA5.5 Ohms-- 40 C+ 105 C2522 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
LQW15AN9N4J0ZD


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 9530
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between Tue. 25 Nov to Thu. 27 Nov
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AUD 0.1117

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Wirewound0402 (1005 METRIC)Unshielded9.4 nH5 %540 mA140 mOhms-- 55 C+ 125 C255.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LQW15AN5N5D10D


RF Inductors - SMD
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Murata 9525
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AUD 0.109

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Wirewound0402 (1005 METRIC)Unshielded5.5 nH0.5 nH800 mA51 mOhms-- 55 C+ 125 C308 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQW15AN3N5C1ZD


RF Inductors - SMD
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Murata 9525
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AUD 0.1302

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Wirewound0402 (1005 METRIC)Unshielded3.5 nH0.2 nH900 mA40 mOhms-- 55 C+ 125 C309.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LQW15AN6N1G8ZD


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 9525
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between Tue. 25 Nov to Thu. 27 Nov
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AUD 0.1535

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Wirewound0402 (1005 METRIC)Unshielded6.1 nH2 %1.6 A56 mOhms-- 55 C+ 125 C88 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
MHQ1005PR27GT000


RF Inductors - SMD IND 0402 270nH S-HQ SMD RF IND
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TDK 9519
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AUD 0.0212

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Multilayer0402 (1005 METRIC)Unshielded270 nH2 %80 mA7 Ohms-- 55 C+ 125 C18900 MHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
LQW15AN7N7G8ZD


RF Inductors - SMD 7.7 NH 2%
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Murata 9519
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AUD 0.1535

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Wirewound0402 (1005 METRIC)Unshielded7.7 nH2 %1.7 A50 mOhms-- 55 C+ 125 C77 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQW15AN5N4G80D


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 9517
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between Tue. 25 Nov to Thu. 27 Nov
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AUD 0.1276

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Wirewound0402 (1005 METRIC)Unshielded5.4 nH2 %1.77 A40 mOhms - 55 C+ 125 C358 GHzStandard1 mm0.6 mm0.5 mm   LQWReel , Cut Tape
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