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
  
                         
NLV25T-8R2J-EF


RF Inductors - SMD 8.2uH 3.05ohms 160mA Wound Ferrite
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TDK 1299
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between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.0515

Multiples of: 10

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded8.2 uH5 %160 mA3.05 Ohms-- 40 C+ 105 C2536 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
S1812R-105K


RF Inductors - SMD 1000uH 10%
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API Delevan 1298
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 4.0142

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RF Choke1812 (4532 METRIC)Shielded1 mH10 %60 mA55 Ohms-- 55 C+ 125 C402 MHzStandard4.8 mm3.4 mm3.4 mm-Ferrite S1812/RReel , Cut Tape
AISC-1210-R39J-T


RF Inductors - SMD FIXED IND 390NH 530MA 580 MOHM
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ABRACON 1294
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.4748

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Wirewound1210 (3225 METRIC)Unshielded390 nH5 %530 mA580 mOhms - 40 C+ 125 C45510 MHzStandard3.65 mm2.95 mm2.7 mm Ceramic AISC - 1210Reel , Cut Tape
AISC-0805-R039J-T


RF Inductors - SMD FIXED IND 39NH 500MA 290 MOHM
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ABRACON 1291
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AUD 0.2823

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Wirewound0805 (2317 METRIC)Unshielded39 nH5 %500 mA290 mOhms - 40 C+ 125 C602 GHzStandard2.29 mm1.73 mm1.55 mm Ceramic AISC - 0805Reel , Cut Tape
AISC-0805F-680J-T


RF Inductors - SMD Inductor Ceramic Core Wire wound 2.3 x 1.7 x 1.55mm
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ABRACON 1287
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AUD 0.2163

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Wirewound0805 (2012 METRIC)Unshielded68 uH5 %40 mA17.5 Ohms - 40 C+ 125 C811 MHzStandard2.29 mm1.73 mm1.55 mm Ferrite AISC - 0805FReel , Cut Tape
LQW15AN5N1C80D


RF Inductors - SMD
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Murata 1276
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1373

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Wirewound0402 (1005 METRIC)Unshielded5.1 nH0.2 nH1.77 A40 mOhms-- 55 C+ 125 C358 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
AIML-0805-120K-T


RF Inductors - SMD FIXED IND 12UH 15MA 1.25 OHM SMD
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ABRACON 1274
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AUD 0.0752

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Multilayer Ferrite Chip Inductor0805 (2012 METRIC)Shielded12 uH10 %15 mA1.25 Ohms - 55 C+ 125 C5022 MHzStandard2 mm1.25 mm0.85 mm Ferrite AIML - 0805Reel , Cut Tape
LQW18ANR15J0ZD


RF Inductors - SMD
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Murata 1272
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AUD 0.1064

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Wirewound0603 (1608 METRIC)Unshielded150 nH5 %160 mA1.5 Ohms-- 55 C+ 125 C321.4 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
AISC-1008-2R7G-T


RF Inductors - SMD FIXED IND 2.7UH 290MA 3.2 OHM
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ABRACON 1266
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AUD 0.0375

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Wirewound1008 (2520 METRIC)Unshielded2.7 uH2 %290 mA3.2 Ohms - 40 C+ 125 C2290 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
LQW18ANR39G8ZD


RF Inductors - SMD .39 UH 2%
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Murata 1266
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.142

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded390 nH2 %190 mA4.23 Ohms-- 55 C+ 125 C301.1 GHzStandard1.65 mm0.99 mm0.9 mm--AEC - Q200LQWReel , Cut Tape
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