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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(Ex. GST)(▲▼)		Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
AISC-1008-3R9J-T


RF Inductors - SMD FIXED IND 3.9UH 260MA 3.6 OHM
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ABRACON 1881
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AUD 0.2876
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Wirewound1008 (2520 METRIC)Unshielded3.9 uH5 %260 mA3.6 Ohms - 40 C+ 125 C1760 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
LQP03TQ1N8B02D


RF Inductors - SMD 1.8nH 650mA 0201 (0603 metric) SUGGESTED ALT LQP03HQ1N8B02D
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Murata 1880
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AUD 0.0293
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Thin Film0201 (0603 METRIC)Unshielded1.8 nH0.1 nH650 mA100 mOhms-- 55 C+ 125 C1715 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
NLV25T-R82J-EFD


RF Inductors - SMD 820nH 1.0ohms 260mA Wound Fer AEC-Q200
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TDK 1877
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AUD 0.1666
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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded820 nH5 %260 mA1 Ohms-- 40 C+ 105 C30260 MHzStandard2.5 mm2 mm1.8 mm-FerriteAEC - Q200NLV25 - EFDReel , Cut Tape
LQW2UAS82NF00L


RF Inductors - SMD 82 NH 1%
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Murata 1874
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AUD 0.3247
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Wirewound1008 (2520 METRIC)Unshielded82 nH1 %1 A220 mOhms-- 55 C+ 125 C601 GHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
NLCV32T-331K-EF


RF Inductors - SMD 330uH 15.99ohms 70mA Wound Ferrite
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TDK 1872
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AUD 0.061
Multiples of: 10

Wirewound1210 (3225 METRIC)Unshielded330 uH10 %70 mA12.3 Ohms-- 40 C+ 105 C206 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFReel , Cut Tape
IMC1008ER2R7J


RF Inductors - SMD 2.7uH 5%
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Vishay 1866
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AUD 0.208
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Wirewound1008 (2520 METRIC)Unshielded2.7 uH5 %195 mA2.6 Ohms-- 40 C+ 125 C20130 MHzStandard2.5 mm2 mm1.6 mm-Ferrite IMCReel , Cut Tape
AS0612N3GTR


RF Inductors - SMD 12.3nH 2% SQUARE AIR CORE
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Kyocera AVX 1865
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AUD 0.337
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Wirewound1.829 mm x 1.397 mm x 1.93 mmUnshielded12.3 nH2 %2.9 A8 mOhms-- 40 C+ 125 C904.8 GHzStandard1.93 mm1.829 mm1.397 mm-Air ASReel , Cut Tape
AISC-1206-R68J-T


RF Inductors - SMD FIXED IND 680NH 430MA 1.58 OHM
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ABRACON 1862
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AUD 0.4308
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Ceramic Wirewound RF Inductor1206 (3216 METRIC)Unshielded680 nH5 %430 mA1.58 Ohms - 40 C+ 125 C45450 MHzStandard3.56 mm2.16 mm1.52 mm Ceramic AISC - 1206Reel , Cut Tape
AISC-0805HQ-12NJ-T


RF Inductors - SMD FIXED IND 12NH 1.6A 45 MOHM SMD
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ABRACON 1861
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AUD 0.3721
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Wirewound0805 (2317 METRIC)Unshielded12 nH5 %1.6 A45 mOhms - 40 C+ 125 C803 GHzStandard2.29 mm1.73 mm1.52 mm Ceramic AISC - 0805HQReel , Cut Tape
NLCV32T-2R2M-EFRD


RF Inductors - SMD 2.2uH 0.115ohm 1.2mA 3.2x2.5mm AEC-Q200
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TDK 1353
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AUD 0.1328
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Wirewound1210 (3225 METRIC)Unshielded2.2 uH20 %770 mA130 mOhms-- 40 C+ 105 C1068 MHzStandard3.2 mm2.5 mm2.4 mm-FerriteAEC - Q200NLCV - EFRDReel , Cut Tape
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