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
  
                         
LQW2UASR33J00L


RF Inductors - SMD .33 UH 5%
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Murata 1299
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AUD 0.1212
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Wirewound1008 (2520 METRIC)Unshielded330 nH5 %450 mA1.05 Ohms-- 55 C+ 125 C45570 MHzStandard2.62 mm2.45 mm1.83 mm-Air LQWReel , Cut Tape
MLF1608DR33MTA00


RF Inductors - SMD 1.6mm x 0.8mm x 0.8mm, -55 to +125 degC, 100mA, 0.33?H, 750mohm
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TDK 1115
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AUD 0.0793
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Multilayer0603 (1608 METRIC)Shielded330 nH20 %100 mA750 mOhms-- 55 C+ 125 C15320 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
IMC1008ERR56J


RF Inductors - SMD 560nH 5%
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Vishay 1115
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AUD 0.1958
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Wirewound1008 (2520 METRIC)Unshielded560 nH5 %310 mA1.5 Ohms-- 40 C+ 125 C45430 MHzStandard2.5 mm2 mm1.6 mm-Ceramic IMCReel , Cut Tape
LQW15AN2N4D10D


RF Inductors - SMD
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Murata 1112
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AUD 0.0844
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Wirewound0402 (1005 METRIC)Unshielded2.4 nH0.5 nH1 A27 mOhms-- 55 C+ 125 C2514 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
AISC-1008-R91G-T


RF Inductors - SMD FIXED IND 910NH 380MA 1.68 OHM
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ABRACON 1112
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AUD 0.3672
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Wirewound1008 (2520 METRIC)Unshielded910 nH2 %380 mA1.68 Ohms - 40 C+ 125 C35295 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
MLF1608DR10KTD25


RF Inductors - SMD 100nH 350mohms 200mA +/-10% Fer AEC-Q200
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TDK 1111
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AUD 0.134
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Multilayer0603 (1608 METRIC)Shielded100 nH10 %200 mA350 mOhms-- 55 C+ 125 C15600 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
B82432C1474K


RF Inductors - SMD SMT-INDUCTOR 1812 470 UH 10%, AEC-Q200
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TDK 1111
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AUD 0.5464
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Wirewound1812 (4532 METRIC)Unshielded470 uH10 %75 mA17.5 Ohms-- 55 C+ 150 C304 MHzStandard4.5 mm3.2 mm3.2 mm-FerriteAEC - Q200B82432CReel , Cut Tape
LQW18CAR16J00D


RF Inductors - SMD Fixed IND 160nH 1300mA NONAUTO
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Murata 1109
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AUD 0.3327
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Wirewound0603 (1608 METRIC)Unshielded160 nH5 %1.3 A75 mOhms-- 55 C+ 125 C331.35 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
MLG1005SR15HTD25


RF Inductors - SMD IND 0402 150nH StdQ AEC Q200 RF IND
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TDK 1067
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AUD 0.0123
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Multilayer inductor  150 nH3 %                
ILSB0805ER8R2K


RF Inductors - SMD 8.2uH 10%
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Vishay 1006
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AUD 0.1293
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Established Reliability0805 (2012 METRIC)Shielded8.2 uH10 %15 mA1.1 Ohms-- 55 C+ 125 C4530 MHzStandard2 mm1.25 mm1.25 mm-  ILSB - 0805Reel , Cut Tape
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