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
  
                         
LQW18ANR20J00D


RF Inductors - SMD 200 NH 5%
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Murata 5682
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0843

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded200 nH5 %120 mA2.4 Ohms-- 55 C+ 125 C251.25 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQW2UAS3R9J00L


RF Inductors - SMD 3.9 UH 5%
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Murata 5681
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1393

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded3.9 uH5 %260 mA3.6 Ohms-- 55 C+ 125 C2070 MHzStandard2.62 mm2.45 mm1.83 mm-Air LQWReel , Cut Tape
PE-1008CLH3R3STS


RF Inductors - SMD 1008 3.3uH 1200mA DCR=182mOhms RF
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Pulse 5673
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2827

Multiples of: 1

Multilayer1008 (2520 METRIC)Shielded3.3 uH-1.2 A175 mOhms650 mA- 40 C+ 85 C-30 MHzStandard2.5 mm2 mm1 mm-Ceramic PE - 1008CLHReel , Cut Tape
B82422A3470K100


RF Inductors - SMD 47nH 510mA 10% 1210 SMD, AEC-Q200
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TDK 5672
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2915

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded47 nH10 %510 mA190 mOhms-- 55 C+ 145 C261.35 GHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422AReel , Cut Tape
LQW18ANR12J0ZD


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 5671
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1064

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded120 nH5 %180 mA1.3 Ohms-- 55 C+ 125 C321.6 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQW15AN5N0B00D


RF Inductors - SMD
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Murata 5665
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.103

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded5 nH0.1 nH600 mA120 mOhms - 55 C+ 125 C258 GHzStandard1 mm0.6 mm0.5 mm   LQWReel , Cut Tape
MHQ0603P3N0ST000


RF Inductors - SMD IND 0201 3.0nH S-HQ SMD RF IND
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TDK 5664
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0949

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded3 nH0.3 nH450 mA300 mOhms-- 55 C+ 125 C1610.3 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
LQG15WHR12J02D


RF Inductors - SMD Fixed IND 120nH 140mA POWRTRN
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Murata 5664
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0949

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Multilayer0402 (1005 METRIC)Unshielded120 nH5 %140 mA2.7 Ohms-- 55 C+ 125 C22800 MHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQW15AN14NG8ZD


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 5664
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1535

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded14 nH2 %1 A111 mOhms-- 55 C+ 125 C315.2 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
MHQ1005P4N3BT000


RF Inductors - SMD IND 0402 4.3nH S-HQ SMD RF IND
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TDK 5659
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0971

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded4.3 nH0.1 nH800 mA100 mOhms - 55 C+ 125 C237.0954 GHzStandard1 mm0.5 mm0.6 mm Ceramic MHQ - PReel , Cut Tape
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