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
  
                         
LQG15HZ2N0S02D


RF Inductors - SMD
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Murata 10544
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.0483

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Multilayer0402 (1005 METRIC)Unshielded2 nH0.3 nH900 mA90 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
AISC-0402-3N9J-T


RF Inductors - SMD FIXED IND 3.9NH 840MA 66 MOHM
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ABRACON 10169
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AUD 0.1776

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Smd Ceramic Wire - Wound Chip Inductors0402 (1005 METRIC)Unshielded3.9 nH5 %840 mA66 mOhms - 40 C+ 125 C206000 MHz     Ceramic Aisc - 0402Reel
LQW15AN6N2D80D


RF Inductors - SMD
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Murata 6867
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AUD 0.1312

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Wirewound0402 (1005 METRIC)Unshielded6.2 nH0.5 nH1.6 A56 mOhms-- 55 C+ 125 C338 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
ATFC-0402-0N4-BT


RF Inductors - SMD Thin Film Chip Inductor 1.0 x 0.5 x 0.32mm
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ABRACON 6866
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.053

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Thin Film Chip Inductor0402 (1005 METRIC)Unshielded400 pH0.1 nH800 mA100 mOhms - 45 C+ 85 C1314 GHzStandard1 mm0.5 mm0.32 mm Ceramic ATFC - 0402Reel , Cut Tape
LQG18HH5N6S00D


RF Inductors - SMD
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Murata 6862
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AUD 0.1382

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Multilayer0603 (1608 METRIC)Unshielded5.6 nH0.3 nH800 mA170 mOhms-- 55 C+ 125 C123 GHzStandard1.6 mm0.8 mm0.8 mm-AirAEC - Q200LQGReel , Cut Tape
MHQ0603P12NHT000


RF Inductors - SMD IND 0201 12nH S-HQ SMD RF IND
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TDK 6857
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AUD 0.0707

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Multilayer0201 (0603 METRIC)Unshielded12 nH3 %240 mA1.4 Ohms-- 55 C+ 125 C164.6 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
LQW18AS47NG00D


RF Inductors - SMD
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Murata 6856
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.0827

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Wirewound0603 (1608 METRIC)Unshielded47 nH2 %600 mA280 mOhms-- 40 C+ 125 C382 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQW18AN37NG80D


RF Inductors - SMD
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Murata 6854
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AUD 0.1098

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Wirewound0603 (1608 METRIC)Unshielded37 nH2 %910 mA200 mOhms-- 55 C+ 125 C373 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
LQW15AN3N7C80D


RF Inductors - SMD
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Murata 6847
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.125

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Wirewound0402 (1005 METRIC)Unshielded3.7 nH0.2 nH1.95 A30 mOhms-- 55 C+ 125 C3510 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LCCI0603J56NGTAR


RF Inductors - SMD 56nH Tol 5% 0603 500 mA DCR=0.75 Ohms
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Kyocera AVX 6833
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AUD 0.0505

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Multilayer0603 (1608 METRIC)Unshielded56 nH5 %500 mA750 mOhms-- 40 C+ 85 C12900 MHzStandard1.6 mm0.8 mm0.8 mm-  LCCIReel , Cut Tape
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