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
  
                         
LQG15WZ2N0S02D


RF Inductors - SMD .3 NH
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Murata 1603
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.0678

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Multilayer0402 (1005 METRIC)Unshielded2 nH0.3 nH1 A50 mOhms-- 55 C+ 125 C238 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
PE-0805CM100JTT


RF Inductors - SMD 10nH 600mA DCR=100mOhms 5%
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Pulse 1597
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.4198

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Multilayer0805 (2012 METRIC)Unshielded10 nH5 %600 mA100 mOhms-- 40 C+ 125 C603.9 GHzStandard2.29 mm1.68 mm1.58 mm-Ceramic PE - 0805CMReel , Cut Tape
NLCV32T-R22M-EFRD


RF Inductors - SMD 0.22uH 0.027ohm 2.4A 3.2x2.5mm AEC-Q200
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TDK 1595
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1553

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Wirewound1210 (3225 METRIC) 220 nH20 %2.4 A32.4 mOhms - 40 C+ 125 C10 Standard3.2 mm2.5 mm2.4 mm FerriteAEC - Q200NLCV - EFRDReel , Cut Tape
ISC1210ER1R0J


RF Inductors - SMD 1uh 5%
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Vishay 1595
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AUD 0.6305

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Molded1210 (3225 METRIC)    15 mOhms     Standard      ISCReel , Cut Tape
NLV32T-150J-EFD


RF Inductors - SMD 15uH 2.8ohms 130mA Wound Fer AEC-Q200
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TDK 1594
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.184

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Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded15 uH5 %130 mA2.8 Ohms-- 40 C+ 105 C3020 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
AS0814N7GTR


RF Inductors - SMD 14.7nH 2% SQUARE AIR CORE
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Kyocera AVX 1590
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.385

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Wirewound2.134 mm x 1.829 mm x 1.549 mmUnshielded14.7 nH2 %4.4 A8 mOhms-- 40 C+ 125 C1303.4 GHzStandard1.549 mm2.134 mm1.829 mm-Air ASReel , Cut Tape
CW252016-82NJ


RF Inductors - SMD 82 NH 5% WIREWOUND
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Bourns 1584
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AUD 0.2045

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Wirewound1008 (2520 METRIC)Unshielded82 nH5 %600 mA180 mOhms-- 40 C+ 125 C601 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
LQW18AS22NJ00D


RF Inductors - SMD
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Murata 1580
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.0761

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Wirewound0603 (1608 METRIC)Unshielded22 nH5 %700 mA190 mOhms-- 40 C+ 125 C383 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
0805F-5R6K-08


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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Fastron 1579
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between Tue. 25 Nov to Mon. 01 Dec
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AUD 0.266

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Wirewound0805 (2012 METRIC)Unshielded5.6 uH10 %175 mA2.8 Ohms - 40 C+ 150 C2080 MHzStandard2.3 mm1.6 mm1.6 mm FerriteAEC - Q2000805FReel
AISC-1008-1R5J-T


RF Inductors - SMD FIXED IND 1.5UH 330MA 2.3 OHM
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ABRACON 1575
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between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.027

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Wirewound1008 (2520 METRIC)Unshielded1.5 uH5 %330 mA2.3 Ohms - 40 C+ 125 C28150 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
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