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
  
                         
LQW18AN58NG80D


RF Inductors - SMD
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Murata 2794
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AUD 0.1312
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Wirewound0603 (1608 METRIC)Unshielded58 nH2 %700 mA300 mOhms-- 55 C+ 125 C352.4 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
ATFC-0402-33N-J-T


RF Inductors - SMD Thin Film Chip Inductor 1.0 x 0.5 x 0.32mm
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ABRACON 2793
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AUD 0.0551
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Thin Film Chip Inductor0402 (1005 METRIC)Unshielded33 nH5 %75 mA4.5 Ohms - 45 C+ 85 C132.5 GHzStandard1 mm0.5 mm0.32 mm Ceramic ATFC - 0402Reel , Cut Tape
LQW15AN6N4C0ZD


RF Inductors - SMD
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Murata 2793
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AUD 0.1293
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Wirewound0402 (1005 METRIC)Unshielded6.4 nH0.2 nH700 mA90 mOhms-- 55 C+ 125 C256 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
B82422T3100K


RF Inductors - SMD SMT-INDUCTOR 1210 0.01 UH 10%,AECQ200
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TDK 2790
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AUD 0.2621
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Wirewound1210 (3225 METRIC)Unshielded10 nH10 %450 mA100 mOhms-- 55 C+ 125 C154 GHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422TReel , Cut Tape
AISC-0805-R56G-T


RF Inductors - SMD FIXED IND 560NH 230MA 1.9 OHM
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ABRACON 2789
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AUD 0.343
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Wirewound0805 (2317 METRIC)Unshielded560 nH2 %230 mA1.9 Ohms - 40 C+ 125 C23320 MHzStandard2.29 mm1.73 mm1.55 mm Ceramic AISC - 0805Reel , Cut Tape
AIMC-Q0603-6N8J-T


RF Inductors - SMD IND 6.8nH 0.7A 250m?
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Abracon 2788
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AUD 0.0854
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Multilayer Ceramic Chip Inductor0603 (1608 METRIC)Shielded6.8 nH5 %700 mA250 mOhms - 55 C+ 125 C104 GHzStandard1.6 mm0.8 mm0.8 mm Ceramic AIMC - Q0603Reel , Cut Tape
MLF2012A2R7J


RF Inductors - SMD 2012 2.7uH 5%
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TDK 2787
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AUD 0.1212
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Multilayer0805 (2012 METRIC)Shielded2.7 uH5 %50 mA550 mOhms-- 55 C+ 125 C45100 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
AIMC-Q0603-1N5S-T


RF Inductors - SMD IND 1.5nH 1A 100m?
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Abracon 2773
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AUD 0.0936
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Multilayer Ceramic Chip Inductor0603 (1608 METRIC)Shielded1.5 nH0.3 nH1 A100 mOhms - 55 C+ 125 C810 GHzStandard1.6 mm0.8 mm0.8 mm Ceramic AIMC - Q0603Reel , Cut Tape
NLV32T-101J-EFD


RF Inductors - SMD 100uH 10ohms 40mA Wound Fer AEC-Q200
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TDK 2698
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AUD 0.1483
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Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded100 uH5 %40 mA10 Ohms-- 40 C+ 105 C2010 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
LQW2BASR12J00L


RF Inductors - SMD .12 UH 5%
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Murata 846
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AUD 0.1069
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Wirewound0805 (2015 METRIC)Unshielded120 nH5 %400 mA510 mOhms-- 55 C+ 125 C501.1 GHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
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