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
  
                         
LCCI0603S3N9GTAR


RF Inductors - SMD 3.9nH Tol 0.3nH 0603 1000mA DCR=0.15 Ohm
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Kyocera AVX 6048
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AUD 0.0271
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Multilayer0603 (1608 METRIC)Unshielded3.9 nH0.3 nH1 A150 mOhms-- 40 C+ 85 C106 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic LCCIReel , Cut Tape
Hot MLF1005VR47JTD25


RF Inductors - SMD 0402 0.47uH 5% AEC-Q200
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TDK 6046
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AUD 0.0488
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Multilayer0402 (1005 METRIC)Shielded470 nH5 %120 mA1.5 Ohms-- 55 C+ 125 C15300 MHzStandard1 mm0.5 mm0.5 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQG15WZ2N3B02D


RF Inductors - SMD Fixed IND 2.3nH 1000mA INFOTMT
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Murata 6043
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AUD 0.142
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Multilayer0402 (1005 METRIC)Unshielded2.3 nH0.1 nH1 A70 mOhms-- 55 C+ 125 C237 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
PM1210-220J-RC


RF Inductors - SMD 22uH 5%
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Bourns 6038
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AUD 0.2365
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Wirewound1210 (3225 METRIC)Unshielded22 uH5 %110 mA3.7 Ohms-- 55 C+ 105 C3020 MHzStandard2.9 mm2.5 mm2.2 mm-Ferrite PM1210Reel , Cut Tape
LQW04AN10NH00D


RF Inductors - SMD
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Murata 6026
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AUD 0.2787
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Wirewound03015 (0804 METRIC)Unshielded10 nH3 %330 mA260 mOhms-- 55 C+ 125 C207 GHzStandard0.8 mm0.4 mm0.4 mm-  LQWReel , Cut Tape
B82422A3100K100


RF Inductors - SMD SMT-INDUCTOR 1210 0.01 UH 10%,AECQ200
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TDK 6024
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AUD 0.3209
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Wirewound1210 (3225 METRIC)Unshielded10 nH10 %750 mA90 mOhms-- 55 C+ 145 C204 GHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422AReel , Cut Tape
L0402R82BHNTR


RF Inductors - SMD 0.82nH +/-0.1nH Tol. SMD 0402
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Kyocera AVX 6022
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AUD 0.3837
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Thin Film0402 (1005 METRIC)Unshielded820 pH0.1 nH500 mA60 mOhms-- 55 C+ 125 C2520 GHzStandard1 mm0.58 mm0.35 mm-  L0402Reel , Cut Tape
AIML-0805-100K-T


RF Inductors - SMD FIXED IND 10UH 15MA 1.15 OHM SMD
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ABRACON 6002
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AUD 0.0806
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Multilayer Ferrite Chip Inductor0805 (2012 METRIC)Shielded10 uH10 %15 mA1.15 Ohms - 55 C+ 125 C5024 MHzStandard2 mm1.25 mm0.85 mm Ferrite AIML - 0805Reel , Cut Tape
AIML-0805HC-2R2M-T


RF Inductors - SMD FIXED IND 2.2UH 1.2A 200 MOHM
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ABRACON 5985
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AUD 0.154
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Multilayer Ferrite Chip Inductor0805 (2012 METRIC)Shielded2.2 uH20 %1.2 A200 mOhms150 mA- 55 C+ 125 C-50 MHzStandard2 mm1.25 mm0.85 mm Ferrite AIML - 0805HCReel , Cut Tape
LQG15HS2N7B02D


RF Inductors - SMD 2.7 NH +/-0.1NH
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Murata 5858
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AUD 0.0338
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Multilayer0402 (1005 METRIC)Unshielded2.7 nH0.1 nH800 mA120 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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