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
  
                         
MLG0603S0N8CT000


RF Inductors - SMD IND 0201 0.8nH StdQ SMD RF IND
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TDK 4287
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0464

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Multilayer0201 (0603 METRIC)Unshielded800 pH0.2 nH600 mA100 mOhms-- 55 C+ 125 C-16.1 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLGReel , Cut Tape
NLCV32T-R15M-EFR


RF Inductors - SMD 150nH 28.8mohms 2.6A 125C Wound Ferrite
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TDK 4275
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1438

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Wirewound1210 (3225 METRIC)Unshielded150 nH20 %2.6 A28.8 mOhms-- 40 C+ 125 C10500 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFRReel , Cut Tape
B82422A1152J100


RF Inductors - SMD SMT-INDUCTOR 1210 1.5UH 5%, AEC-Q200
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TDK 4274
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AUD 0.3172

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Wirewound1210 (3225 METRIC)Unshielded1.5 uH5 %340 mA500 mOhms-- 55 C+ 145 C20270 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
HL023R0BTTR


RF Inductors - SMD 3.0nH
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Kyocera AVX 4270
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AUD 0.3408

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Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded3 nH0.1 nH200 mA300 mOhms-- 55 C+ 125 C157 GHzStandard1 mm0.58 mm0.35 mm-  HLReel , Cut Tape
LQW15CNR22J10D


RF Inductors - SMD
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Murata 4263
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between Fri. 21 Nov to Thu. 27 Nov
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AUD 0.0752

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Wirewound0402 (1005 METRIC)Unshielded220 nH5 %450 mA470 mOhms-- 55 C+ 125 C-1.4 GHzStandard1 mm0.6 mm0.5 mm-Ferrite LQWReel , Cut Tape
L04021R0AHNTR


RF Inductors - SMD 1nH
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Kyocera AVX 4254
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.6381

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Thin Film0402 (1005 METRIC)Unshielded1 nH0.05 nH500 mA150 mOhms-- 55 C+ 125 C2020 GHzStandard1 mm0.58 mm0.35 mm-  L0402Reel , Cut Tape
NLV25T-R15J-EF


RF Inductors - SMD 150nH 350mohms 500mA Wound Ferrite
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TDK 4251
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1339

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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded150 nH5 %500 mA350 mOhms-- 40 C+ 105 C30550 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
LQW18AN25NJ8ZD


RF Inductors - SMD
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Murata 4240
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1382

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Wirewound0603 (1608 METRIC)Unshielded25 nH5 %1.2 A98 mOhms-- 55 C+ 125 C403.6 GHzStandard1.65 mm0.99 mm0.9 mm- AEC - Q200LQWReel , Cut Tape
IMC1008ER47NJ


RF Inductors - SMD 47nH 5%
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Vishay 4237
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1855

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Wirewound1008 (2520 METRIC)Unshielded47 nH5 %1 A100 mOhms-- 40 C+ 125 C601.5 GHzStandard2.5 mm2 mm1.6 mm-Ceramic IMCReel , Cut Tape
CS160808-1R0K


RF Inductors - SMD 1.0uH 10%
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Bourns 4226
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0752

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Multilayer0603 (1608 METRIC)Shielded1 uH10 %100 mA500 mOhms-- 55 C+ 125 C5070 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite  Reel , Cut Tape
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