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
  
                         
AIAC-0805C-4N7K-T


RF Inductors - SMD FIXED IND 4.7NH 900MA 3.6 MOHM
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ABRACON 2221
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.715

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SMT Air Coil Inductor0805 (2012 METRIC)Unshielded4.7 nH10 %900 mA3.6 mOhms - 40 C+ 125 C803 GHzStandard2.85 mm1.8 mm2.1 mm Air AIAC - 0805CReel , Cut Tape
MHQ0603P7N5JT000


RF Inductors - SMD IND 0201 7.5nH S-HQ SMD RF IND
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TDK 2216
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.0667

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Multilayer0201 (0603 METRIC)Unshielded7.5 nH5 %300 mA500 mOhms-- 55 C+ 125 C165.7 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
LQW2UAS68NF00L


RF Inductors - SMD 68 NH 1%
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Murata 2205
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.2973

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Wirewound1008 (2520 METRIC)Unshielded68 nH1 %1 A200 mOhms-- 55 C+ 125 C651.3 GHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
LQW18AN62NJ0ZD


RF Inductors - SMD
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Murata 2193
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1293

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Wirewound0603 (1608 METRIC)Unshielded62 nH5 %280 mA51 mOhms-- 55 C+ 125 C382.3 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
HLC022R0BTTR


RF Inductors - SMD 2.0nH
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Kyocera AVX 2167
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.2035

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Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded2 nH0.1 nH596 mA180 mOhms-- 55 C+ 125 C2617 GHzStandard1 mm0.58 mm0.35 mm-  HLCReel , Cut Tape
5406 220 34 00


RF Inductors - SMD RF Chip Inductor SMD 22nH 0603 5% Tol
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Sumida 2164
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.3614

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RF Choke0603 (1608 METRIC)Unshielded22 nH5 %450 mA135 mOhms-- 55 C+ 125 C453.1 GHzStandard1.7 mm1.2 mm0.85 mm-Ceramic 5406Reel , Cut Tape
LQG15WH4N7B02D


RF Inductors - SMD
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Murata 2163
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1504

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded4.7 nH0.1 nH800 mA110 mOhms-- 55 C+ 125 C235 GHzStandard1 mm0.6 mm0.5 mm-Air LQGReel , Cut Tape
MHQ0603P2N9BTD25


RF Inductors - SMD 0201 2.9nH Tol 0.1nH AEC-Q200
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TDK 2158
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.0709

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Multilayer0201 (0603 METRIC)Unshielded2.9 nH0.1 nH450 mA300 mOhms-- 55 C+ 125 C1610.8 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
MCL1608V1-100-R


RF Inductors - SMD 10 UH 20%
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Eaton 2156
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.0642

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Multilayer0603 (1608 METRIC)Unshielded10 uH20 %60 mA1.15 Ohms-- 40 C+ 85 C-17 MHzStandard1.6 mm0.8 mm0.8 mm-  MCLReel , Cut Tape
AS0816N6GTR


RF Inductors - SMD 16.6nH 2% SQUARE AIR CORE
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Kyocera AVX 2153
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.3714

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   16.6 nH2 %2.9 A8 mOhms - 40 C+ 125 C604.9 GHzStandard2.21 mm2.134 mm1.829 mm   ASReel , Cut Tape
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