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
  
                         
PE-0603CD220GTT


RF Inductors - SMD SMD IND
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Pulse 2361
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.2695

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Multilayer0603 (1608 METRIC)Unshielded22 nH2 %700 mA190 mOhms-- 40 C+ 125 C353 GHzStandard1.8 mm1.24 mm1.02 mm-Ceramic CDReel , Cut Tape
AISC-0603-R0062J-T


RF Inductors - SMD FIXED IND 6.2NH 700MA 95 MOHM
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ABRACON 2341
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AUD 0.1485

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Wirewound0603 (1812 METRIC)Unshielded6.2 nH5 %700 mA95 mOhms - 40 C+ 125 C296 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - 0603Reel , Cut Tape
MLF1608E6R8KTD25


RF Inductors - SMD 6.8uH 1.3ohms 15mA +/-10% Fer AEC-Q200
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TDK 2338
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AUD 0.1208

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Multilayer0603 (1608 METRIC)Shielded6.8 uH10 %15 mA1.3 Ohms-- 55 C+ 125 C3560 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
CW252016-R82J


Inductor RF Wirewound 0.82uH 5% 25.2MHz 45Q-Factor Ceramic 0.18A 2.3Ohm DCR 1008 T/R
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Bourns 2328
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AUD 0.1836

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Wirewound1008 (2520 METRIC)Unshielded820 nH5 %360 mA1.61 Ohms-- 40 C+ 125 C45350 MHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
ILSB0603ER6R8K


RF Inductors - SMD 6.8uH 10%
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Vishay 2327
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AUD 0.1232

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Established Reliability0603 (1608 METRIC)Shielded6.8 uH10 %15 mA1.7 Ohms-- 55 C+ 125 C3020 MHzStandard1.6 mm0.8 mm0.8 mm-  ILSB - 0603Reel , Cut Tape
LQW18ANR22J0ZD


RF Inductors - SMD
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Murata 2325
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AUD 0.1064

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Wirewound0603 (1608 METRIC)Unshielded220 nH5 %120 mA2.5 Ohms-- 55 C+ 125 C251.2 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
0805F100K01


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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Fastron 2315
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AUD 0.2787

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Wirewound0805 (2012 METRIC)Unshielded10 uH10 %150 mA3.8 Ohms-- 40 C+ 150 C2045 MHzStandard2.3 mm1.6 mm1.6 mm-FerriteAEC - Q2000805FReel , Cut Tape
AIML-0805-220K-T


RF Inductors - SMD FIXED IND 22UH 5MA 1.1 OHM SMD
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ABRACON 2311
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AUD 0.0806

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Multilayer Ferrite Chip Inductor0805 (2012 METRIC)Shielded22 uH10 %5 mA1.1 Ohms - 55 C+ 125 C3016 MHzStandard2 mm1.25 mm0.85 mm Ferrite AIML - 0805Reel , Cut Tape
LQW18AS23NG00D


RF Inductors - SMD
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Murata 2308
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.0947

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded23 nH2 %700 mA190 mOhms - 40 C+ 125 C382.85 GHzStandard1.6 mm0.8 mm0.8 mm   LQWReel , Cut Tape
MHQ1005P5N6CT000


RF Inductors - SMD IND 0402 5.6nH S-HQ SMD RF IND
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TDK 1765
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between Mon. 08 Dec to Thu. 11 Dec
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AUD 0.0139

Multiples of: 20

Multilayer0402 (1005 METRIC)Unshielded5.6 nH0.2 nH800 mA130 mOhms-- 55 C+ 125 C236.5 GHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
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