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-0603-R072J-T


RF Inductors - SMD FIXED IND 72NH 320MA 430 MOHM
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ABRACON 2420
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AUD 0.1655
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Wirewound0603 (1812 METRIC)Unshielded72 nH5 %320 mA430 mOhms - 40 C+ 125 C342.1 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - 0603Reel , Cut Tape
LQW2UAS68NG00L


RF Inductors - SMD
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Murata 1823
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AUD 0.1534
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Wirewound1008 (2520 METRIC)Unshielded68 nH2 %1 A200 mOhms-- 55 C+ 125 C651.3 GHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
CC453232-391KL


RF Inductors - SMD 390uH 10% 796KHz
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Bourns 1822
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AUD 0.22
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Wirewound1812 (4532 METRIC) 390 uH10 %85 mA14 Ohms - 40 C+ 125 C203 MHzStandard4.2 mm3.2 mm3.2 mm   CC453232Reel , Cut Tape
CMH322522-1R2KL


RF Inductors - SMD 1.2uH 10% 7.96MHz
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Bourns 1821
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AUD 0.418
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Wirewound1210 (3225 METRIC)Shielded1.2 uH10 %390 mA750 mOhms-- 55 C+ 125 C30100 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite  Reel , Cut Tape
ILSB1206ER150K


RF Inductors - SMD 15uH 10%
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Vishay 1816
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AUD 0.1636
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Established Reliability1206 (3216 METRIC)Shielded15 uH10 %5 mA700 mOhms-- 55 C+ 125 C4522 MHzStandard3.2 mm1.6 mm1.1 mm-  ILSB - 1206Reel , Cut Tape
AISC-1008HQ-12NJ-T


RF Inductors - SMD FIXED IND 12NH 1.5A 60 MOHM SMD
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Abracon 1816
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AUD 0.1999
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Wirewound1008 (2520 METRIC)Unshielded12 nH5 %1.5 A60 mOhms - 40 C+ 125 C702.8 GHzStandard2.6 mm2.1 mm1.7 mm Ceramic AISC - 1008HQReel , Cut Tape
4310LC-132KEC


RF Inductors - SMD 4310 1.3uH Unshld 10% 15.1mOhms
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Coilcraft 1813
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AUD 4.2426
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Wideband Bias Choke4.826 mm x 3.3 mm x 11.68 mmUnshielded1.3 uH10 %4.2 A15.1 mOhms-- 40 C+ 85 C-235 MHzStandard11.68 mm4.826 mm3.3 mm-Ferrite 4310LCReel , Cut Tape
NLFV32T-150K-EF


RF Inductors - SMD 3.2mm x 2.5mm x 2.2mm, -40 to +105 degC, 140mA, 15?H, 360mohm
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TDK 1810
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AUD 0.2103
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Wirewound1210 (3225 METRIC)Shielded15 uH10 %140 mA300 mOhms-- 40 C+ 105 C--Standard3.2 mm2.5 mm2.2 mm-Ferrite NLFV32 - EFReel , Cut Tape
AISC-0603-R022G-T


RF Inductors - SMD FIXED IND 22NH 490MA 190 MOHM
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ABRACON 1810
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AUD 0.162
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Wirewound0603 (1812 METRIC)Unshielded22 nH2 %490 mA190 mOhms - 40 C+ 125 C384.6 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - 0603Reel , Cut Tape
IMC1008ER82NJ


RF Inductors - SMD 82nH 5%
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Vishay 1593
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AUD 0.1827
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Wirewound1008 (2520 METRIC)Unshielded82 nH5 %1 A180 mOhms-- 40 C+ 125 C601.1 GHzStandard2.5 mm2 mm1.6 mm-Ceramic IMCReel , Cut Tape
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