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
  
                         
CS160808-R18K


RF Inductors - SMD 0.18uH '10%
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Bourns 2976
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0827

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Multilayer0603 (1608 METRIC)Shielded180 nH10 %200 mA400 mOhms-- 55 C+ 125 C30165 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite  Reel , Cut Tape
LQW15AN5N9B8ZD


RF Inductors - SMD
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Murata 2968
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1401

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded5.9 nH0.1 nH1.77 A40 mOhms-- 55 C+ 125 C308 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
CW252016-2R7J


RF Inductors - SMD 2.7 UH 5%
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Bourns 2964
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1799

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded2.7 uH5 %195 mA3.2 Ohms-- 40 C+ 125 C22195 MHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
NLCV32T-100K-EFR


RF Inductors - SMD 10uH 504mohms 600mA 125C Wound Ferrite
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TDK 2963
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.1238

Multiples of: 5

Wirewound1210 (3225 METRIC)Unshielded10 uH10 %450 mA360 mOhms-- 40 C+ 105 C1530 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFRReel , Cut Tape
LQW18AN16NJ0ZD


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 2958
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1293

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded16 nH5 %550 mA160 mOhms-- 55 C+ 125 C405.5 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
CW201212-R82J


RF Inductors - SMD 820nH 5% HIGH Q
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Bourns 2945
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2108

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Wirewound0805 (2012 METRIC)Unshielded820 nH5 %180 mA2.35 Ohms-- 40 C+ 125 C601.3 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW201212Reel , Cut Tape
5508 470 34 00


RF Inductors - SMD RF Chip Inductor SMD 47nH 0805 5% Tol
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Sumida 2943
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.418

Multiples of: 1

RF Choke0805 (2012 METRIC)Unshielded47 nH5 %500 mA130 mOhms-- 55 C+ 125 C451.9 GHzStandard2.2 mm1.4 mm1.42 mm-Ceramic 5508Reel , Cut Tape
NLCV25T-R15M-EFR


RF Inductors - SMD 150nH 52.8mohms 1.8A 125C Wound Ferrite
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TDK 2938
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1287

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded150 nH20 %1.8 A44 mOhms-- 40 C+ 125 C5-Standard2.5 mm2 mm1.8 mm-Ferrite NLCV - EFRReel , Cut Tape
AISC-1206-R39J-T


RF Inductors - SMD FIXED IND 390NH 530MA 800 MOHM
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ABRACON 2937
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.4602

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Ceramic Wirewound RF Inductor1206 (3216 METRIC)Unshielded390 nH5 %530 mA800 mOhms - 40 C+ 125 C45600 MHzStandard3.56 mm2.16 mm1.52 mm Ceramic AISC - 1206Reel , Cut Tape
MLG0603S27NJT000


RF Inductors - SMD IND 0201 27nH StdQ SMD RF IND
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TDK 2489
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0403

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Multilayer0201 (0603 METRIC)Unshielded27 nH5 %100 mA1.5 Ohms-- 55 C+ 125 C62.2 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLGReel , Cut Tape
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