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
  
                         
AISC-0805-R068J-T


RF Inductors - SMD FIXED IND 68NH 500MA 380 MOHM
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ABRACON 1810
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between Mon. 08 Dec to Thu. 11 Dec
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AUD 0.2736

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Wirewound0805 (2317 METRIC)Unshielded68 nH5 %500 mA380 mOhms - 40 C+ 125 C551.45 GHzStandard2.29 mm1.73 mm1.55 mm Ceramic AISC - 0805Reel , Cut Tape
AISC-1210-3R0J-T


RF Inductors - SMD FIXED IND 3UH 300MA 3.12 OHM SMD
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ABRACON 1810
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.4748

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Wirewound1210 (3225 METRIC)Unshielded3 uH5 %300 mA3.12 Ohms - 40 C+ 125 C20110 MHzStandard3.65 mm2.95 mm2.7 mm Ceramic AISC - 1210Reel , Cut Tape
AISC-0805-R056G-T


RF Inductors - SMD FIXED IND 56NH 500MA 320 MOHM
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ABRACON 1809
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AUD 0.2823

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Wirewound0805 (2317 METRIC)Unshielded56 nH2 %500 mA320 mOhms - 40 C+ 125 C551.55 GHzStandard2.29 mm1.73 mm1.55 mm Ceramic AISC - 0805Reel , Cut Tape
NLV25T-3R9J-EFD


RF Inductors - SMD 3.9uH 2.1ohms 180mA Wound Fer AEC-Q200
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TDK 1806
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AUD 0.1258

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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded3.9 uH5 %180 mA2.1 Ohms-- 40 C+ 105 C3048 MHzStandard2.5 mm2 mm1.8 mm-FerriteAEC - Q200NLV25 - EFDReel , Cut Tape
IMC0805ER8R2J01


RF Inductors - SMD 8.2uH 5%
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Vishay 1804
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AUD 0.2201

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Wirewound0805 (2012 METRIC)Unshielded8.2 nH5 %600 mA60 mOhms-- 40 C+ 125 C605.5 GHzStandard2 mm1.25 mm1.2 mm-Ceramic IMCReel , Cut Tape
AISC-1206-27NJ-T


RF Inductors - SMD FIXED IND 27NH 1A 120 MOHM SMD
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ABRACON 1803
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AUD 0.2787

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Ceramic Wirewound RF Inductor1206 (3216 METRIC)Unshielded27 nH5 %1 A120 mOhms - 40 C+ 125 C501.8 GHzStandard3.56 mm2.16 mm1.52 mm Ceramic AISC - 1206Reel , Cut Tape
CMH322522-R22ML


RF Inductors - SMD MAGNETICS - CHIP INDUCTOR
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Bourns 1803
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AUD 0.422

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Wirewound1210 (3225 METRIC)Shielded1.5 nH20 %450 mA320 mOhms-- 55 C+ 125 C30350 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite CMH322522Reel , Cut Tape
LQG15WZ6N8G02D


RF Inductors - SMD
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Murata 1796
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AUD 0.1456

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Multilayer0402 (1005 METRIC)Unshielded6.8 nH2 %700 mA140 mOhms-- 55 C+ 125 C234 GHzStandard1 mm0.6 mm0.5 mm Air LQGReel , Cut Tape
AISC-1008F-1R8J-T


RF Inductors - SMD Inductor Ceramic Core Wire wound 2.9 x 2.8 x 2.3mm
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ABRACON 1794
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AUD 0.293

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Wirewound1008 (2520 METRIC)Unshielded1.8 uH5 %600 mA840 mOhms - 40 C+ 125 C33170 MHzStandard2.92 mm2.79 mm2.29 mm Ferrite AISC - 1008FReel , Cut Tape
NLCV32T-220K-EF


RF Inductors - SMD 22uH 1.001ohms 300mA Wound Ferrite
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TDK 601
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AUD 0.0414

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Wirewound1210 (3225 METRIC)Unshielded22 uH10 %300 mA770 mOhms-- 40 C+ 105 C1521 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFReel , Cut Tape
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