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
  
                         
LQG18HH12NJ00D


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 3310
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1339

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Multilayer0603 (1608 METRIC)Unshielded12 nH5 %600 mA300 mOhms-- 55 C+ 125 C122.2 GHzStandard1.6 mm0.8 mm0.8 mm-AirAEC - Q200LQGReel , Cut Tape
PM0603-10NJ-RC


10 nH Unshielded Drum Core, Wirewound Inductor 700 mA 130mOhm 0603 (1608 Metric)
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Bourns 3307
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1925

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Wirewound0603 (1608 METRIC)Unshielded10 nH5 %700 mA150 mOhms-- 40 C+ 125 C304.8 GHzStandard1.65 mm1.05 mm1 mm-Alumina PM0603Reel , Cut Tape
ILSB0805ERR82K


RF Inductors - SMD .82uH 10%
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Vishay 3304
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AUD 0.1252

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Established Reliability0805 (2012 METRIC)Shielded820 nH10 %150 mA1 Ohms-- 55 C+ 125 C25115 MHzStandard2 mm1.25 mm0.9 mm-  ILSB - 0805Reel , Cut Tape
NLV25T-2R7J-EF


RF Inductors - SMD 2.7uH 1.7ohms 195mA Wound Ferrite
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TDK 3300
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AUD 0.1485

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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded2.7 uH5 %195 mA1.7 Ohms-- 40 C+ 105 C3070 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
AISC-0603-R12J-T


RF Inductors - SMD FIXED IND 120NH 240MA 750 MOHM
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ABRACON 3299
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AUD 0.1485

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Wirewound0603 (1812 METRIC)Unshielded120 nH5 %240 mA750 mOhms - 40 C+ 125 C321.6 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - 0603Reel , Cut Tape
MLF1608C220MTD25


RF Inductors - SMD 22uH 1.7ohms 2mA +/-20% Fer AEC-Q200
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TDK 3298
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1454

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Multilayer0603 (1608 METRIC)Shielded22 uH20 %2 mA1.7 Ohms-- 55 C+ 125 C2038 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
AISC-1008F-1R8G-T


RF Inductors - SMD FIXED IND 1.8UH 600MA 840 MOHM
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ABRACON 3290
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AUD 0.2438

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Wirewound1008 (2520 METRIC)Unshielded1.8 uH2 %600 mA840 mOhms - 40 C+ 125 C33170 MHzStandard2.92 mm2.79 mm2.29 mm Ferrite AISC - 1008FReel , Cut Tape
0603AS-8N2J-01


RF Inductors - SMD Wire-wound Ceramic RF Chip Inductor
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Fastron 3289
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AUD 0.2076

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Wirewound0603 (1608 METRIC)Unshielded8.2 nH5 %700 mA120 mOhms - 40 C+ 150 C305.4 GHzStandard1.7 mm1.1 mm1 mm CeramicAEC - Q2000603ASReel , Cut Tape
MLF1608A1R0MTD25


RF Inductors - SMD 1.0uH 500mohms 50mA +/-20% Fer AEC-Q200
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TDK 3288
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1283

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Multilayer0603 (1608 METRIC)Shielded1 uH20 %50 mA500 mOhms-- 55 C+ 125 C35170 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQW18AN16NG00D


RF Inductors - SMD 16 NH 2%
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Murata 679
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.045

Multiples of: 20

Wirewound0603 (1608 METRIC)Unshielded16 nH2 %550 mA160 mOhms-- 55 C+ 125 C405.5 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
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