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
  
                         
0805AS-R47J-01


RF Inductors - SMD 470nH 100 MHz 5% Tol
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Fastron 2415
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AUD 0.1931
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Wirewound0805 (2012 METRIC)Unshielded470 nH5 %170 mA2.5 Ohms-- 40 C+ 150 C40720 MHzStandard2.3 mm1.8 mm1.6 mm-CeramicAEC - Q2000805ASReel , Cut Tape
0805AQ-016G-01


RF Inductors - SMD 16nH 250 MHz 2% tol
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Fastron 2415
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AUD 0.2099
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Wirewound0805 (2012 METRIC)Unshielded16 nH2 %1.5 A60 mOhms-- 40 C+ 150 C782.95 GHzStandard2.3 mm1.8 mm1.6 mm-CeramicAEC - Q2000805AQReel , Cut Tape
LQP02HQ3N6B02E


RF Inductors - SMD
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Murata 2410
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AUD 0.1192
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Thin Film01005 (0402 METRIC)Unshielded3.6 nH0.1 nH350 mA300 mOhms-- 55 C+ 125 C148.2 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , Cut Tape
L0805120GEWTR


RF Inductors - SMD 12nH 2%
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Kyocera AVX 2405
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AUD 0.8844
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Thin Film0805 (2012 METRIC)Unshielded12 nH2 %1.5 A200 mOhms-- 55 C+ 125 C402.4 GHzStandard2.11 mm1.5 mm0.91 mm-  0603, 0805Reel , Cut Tape
MLF1608E120MTD00


RF Inductors - SMD 1.6mm x 0.8mm x 0.8mm, -55 to +125 degC, 10mA, 12?H, 1.8ohm
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TDK 2404
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AUD 0.08
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Multilayer Unshielded12 uH20 %10 mA1.8 Ohms-- 55 C+ 125 C-45 MHzStandard1.6 mm0.8 mm0.95 mm-Ferrite MLFReel , Cut Tape
0805AS027J01


RF Inductors - SMD Wire-wound Ceramic RF Chip Inductor
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Fastron 2398
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AUD 0.1862
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Wirewound0805 (2012 METRIC)Unshielded27 nH5 %500 mA250 mOhms - 40 C+ 150 C552.5 GHzStandard2.3 mm1.8 mm1.6 mm-CeramicAEC - Q2000805ASReel , Cut Tape
MHQ0603P5N6HT000


RF Inductors - SMD IND 0201 5.6nH S-HQ SMD RF IND
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TDK 2392
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AUD 0.016
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Multilayer0201 (0603 METRIC)Unshielded5.6 nH3 %350 mA400 mOhms-- 55 C+ 125 C167.1 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
LQG15HH2N4S02D


RF Inductors - SMD
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Murata 2391
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AUD 0.0971
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Multilayer0402 (1005 METRIC)Unshielded2.4 nH0.3 nH850 mA110 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQW15AN1N4C10D


1.4nH 19mO 0402 Inductors (SMD) ROHS
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Murata 1416
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AUD 0.0473
Multiples of: 10

Wirewound0402 (1005 METRIC)Unshielded1.4 nH0.2 nH1.1 A19 mOhms-- 55 C+ 125 C2515 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
PM1210-2R2J-RC


Inductor RF Molded Bobbin Core 2.2uH 5% 7.96MHz 30Q-Factor Ferrite 0.32A 1Ohm DCR 1210 T/R
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Bourns 463
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AUD 0.242
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Wirewound1210 (3225 METRIC)Unshielded2.2 uH5 %320 mA1 Ohms-- 55 C+ 105 C3075 MHzStandard2.9 mm2.5 mm2.2 mm-Ferrite PM1210Reel , Cut Tape
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