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
  
                         
LQW18ANR13J0ZD


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 2723
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1212

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Wirewound0603 (1608 METRIC)Unshielded130 nH5 %170 mA1.4 Ohms-- 55 C+ 125 C321.45 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
ILSB0603ER47NM


RF Inductors - SMD .047uH 20%
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Vishay 2721
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AUD 0.105

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Established Reliability0603 (1608 METRIC)Shielded470 nH10 %35 mA1.35 Ohms-- 55 C+ 125 C15121 MHzStandard1.6 mm0.8 mm0.8 mm-  ILSB - 0603Reel , Cut Tape
LQW15AN6N8J8ZD


RF Inductors - SMD
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Murata 2714
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AUD 0.1352

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Wirewound0402 (1005 METRIC)Unshielded6.8 nH5 %1.45 A68 mOhms-- 55 C+ 125 C307 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
AISC-0603-R22J-T


RF Inductors - SMD FIXED IND 220NH 140MA 2.1 OHM
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ABRACON 2714
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AUD 0.1888

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Wirewound0603 (1812 METRIC)Unshielded220 nH5 %140 mA2.1 Ohms - 40 C+ 125 C251.2 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - 0603Reel , Cut Tape
MLF1005GR39JT000


RF Inductors - SMD 1mm x 0.5mm x 0.5mm, -55 to +125 degC, 50mA, 0.39?H, 410mohm
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TDK 2711
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AUD 0.1614

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Multilayer0402 (1005 METRIC)Shielded390 nH5 %50 mA410 mOhms-- 55 C+ 125 C30600 MHzStandard1 mm0.5 mm0.5 mm-Ferrite MLFReel , Cut Tape
MHL1ECTTP18NJ


RF Inductors - SMD 18nH 5%
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KOA Speer 2710
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AUD 0.1155

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Multilayer0402 (1005 METRIC)Unshielded18 nH5 %250 mA650 mOhms-- 55 C+ 125 C82.9 GHzStandard1 mm0.5 mm0.5 mm-Ceramic MHLReel , Cut Tape
CW252016-R10J


Inductor RF Wirewound 0.1uH 5% 25.2MHz 60Q-Factor Ceramic 0.65A 0.56Ohm DCR 1008 T/R
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Bourns 2709
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AUD 0.1738

Multiples of: 2000

Wirewound1008 (2520 METRIC)Unshielded100 nH5 %500 mA180 mOhms-- 40 C+ 125 C601 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
IMC1812ES2R7K


RF Inductors - SMD 2.7uH 10%
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Vishay 2706
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AUD 0.5737

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Wirewound1812 (4532 METRIC)Unshielded2.7 uH10 %370 mA750 mOhms-- 55 C+ 125 C5050 MHzStandard4.5 mm3.2 mm3.2 mm-  IMCReel , Cut Tape
LQW18ANR22G0ZD


RF Inductors - SMD
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Murata 2705
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AUD 0.1155

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Wirewound0603 (1608 METRIC)Unshielded220 nH2 %120 mA2.5 Ohms-- 55 C+ 125 C251.2 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
AISC-0603-R082G-T


RF Inductors - SMD FIXED IND 82NH 300MA 500 MOHM
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ABRACON 2705
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AUD 0.1907

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Wirewound0603 (1812 METRIC)Unshielded82 nH2 %300 mA500 mOhms - 40 C+ 125 C342 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - 0603Reel , Cut Tape
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