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-Q0402-12NG-T


RF Inductors - SMD IND 12nH 0.64A 120m?
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Abracon 3880
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AUD 0.1638
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded12 nH2 %640 mA120 mOhms - 40 C+ 125 C243.6 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
AISC-Q0402-11NG-T


RF Inductors - SMD IND 11nH 0.64A 120m?
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AUD 0.1638
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded11 nH2 %640 mA120 mOhms - 40 C+ 125 C243.68 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
AISC-Q0402-15NG-T


RF Inductors - SMD IND 15nH 0.56A 172m?
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AUD 0.1638
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded15 nH2 %560 mA172 mOhms - 40 C+ 125 C243.28 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
BWLM00181009R16J00


RF Inductors - SMD Chilisin RF inductor Wire Wound-STD
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Pulse 3880
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AUD 0.1676
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 1.8 mm x 1 mm x 0.9 mmUnshielded160 nH5 %1 A100 mOhms - 40 C+ 125 C 900 MHzStandard1.8 mm1 mm0.9 mm Ferrite BWLMReel , Cut Tape
AISC-1210HS-2R2K-T2


RF Inductors - SMD FIXED IND 2.2UH 800MA 500 MOHM
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ABRACON 3880
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AUD 0.1706
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Wirewound1210 (3225 METRIC)Unshielded2.2 uH10 %800 mA500 mOhms850 mA- 40 C+ 85 C10150 MHzStandard3.2 mm3.05 mm1.3 mm Ferrite AISC - 1210HSReel , Cut Tape
MHQ1005PR15JTD25


RF Inductors - SMD IND 0402 150nH S-HQ AEC Q200 RF IND
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TDK 3880
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AUD 0.1838
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Multilayer0402 (1005 METRIC)Unshielded150 nH5 %110 mA3 Ohms-- 55 C+ 125 C221 GHzStandard1 mm0.5 mm0.6 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
AISC-Q0603HQ-10NG-T


RF Inductors - SMD IND 10nH 1.4A 48m?
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Abracon 3880
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AUD 0.1962
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Wirewound0603 (1812 METRIC)Unshielded10 nH2 %1.4 A48 mOhms - 40 C+ 125 C494.3 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - Q0603HQReel , Cut Tape
AISC-Q0603HQ-33NG-T


RF Inductors - SMD IND 33nH 0.68A 170m?
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AUD 0.1962
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Wirewound0603 (1812 METRIC)Unshielded33 nH2 %680 mA170 mOhms - 40 C+ 125 C452.7 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - Q0603HQReel , Cut Tape
AISC-Q0603HQ-22NG-T


RF Inductors - SMD IND 22nH 0.85A 140m?
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Abracon 3880
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AUD 0.1962
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Wirewound0603 (1812 METRIC)Unshielded22 nH2 %850 mA140 mOhms - 40 C+ 125 C443.15 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - Q0603HQReel , Cut Tape
AISC-Q0603HQ-27NG-T


RF Inductors - SMD IND 27nH 0.78A 150m?
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AUD 0.1962
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Wirewound0603 (1812 METRIC)Unshielded27 nH2 %780 mA150 mOhms - 40 C+ 125 C442.8 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - Q0603HQReel , Cut Tape
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