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
  
                         
IMC1008ER18NJ


RF Inductors - SMD 18nH 5%
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Vishay 3140
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AUD 0.1958
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Wirewound1008 (2520 METRIC)Unshielded18 nH5 %1 A100 mOhms-- 40 C+ 125 C602.7 GHzStandard2.5 mm2 mm1.6 mm-Ceramic IMCReel , Cut Tape
IMC1008ER8R2J


RF Inductors - SMD 8.2uH 5%
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Vishay 3132
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AUD 0.2181
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Wirewound1008 (2520 METRIC)Unshielded8.2 uH5 %160 mA3.05 Ohms-- 40 C+ 125 C2036 MHzStandard2.5 mm2 mm1.6 mm-Ferrite IMCReel , Cut Tape
LQW2BASR12G00L


RF Inductors - SMD 120 NH 2%
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Murata 3128
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AUD 0.1339
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Wirewound0805 (2015 METRIC)Unshielded120 nH2 %400 mA510 mOhms-- 55 C+ 125 C501.1 GHzStandard2.09 mm1.53 mm1.42 mm-- LQW2BAReel , Cut Tape
MLF2012DR10KTD25


RF Inductors - SMD 100nH 150mohms 300mA +/-10% Fer AEC-Q200
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TDK 3126
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AUD 0.142
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Multilayer0805 (2012 METRIC)Shielded100 nH10 %300 mA150 mOhms-- 55 C+ 125 C20500 MHzStandard2 mm1.25 mm0.85 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQW18AN36NJ8ZD


RF Inductors - SMD
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Murata 3125
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AUD 0.1493
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Wirewound0603 (1608 METRIC)Unshielded36 nH5 %910 mA200 mOhms-- 55 C+ 125 C373 GHzStandard1.65 mm0.99 mm0.9 mm- AEC - Q200LQWReel , Cut Tape
LQW18AN30NJ0ZD


RF Inductors - SMD
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Murata 3120
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AUD 0.1212
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Wirewound0603 (1608 METRIC)Unshielded30 nH5 %420 mA230 mOhms-- 55 C+ 125 C403.3 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
CWF2414-1R0K


RF Inductors - SMD Ind,2.2x1.4x1.3mm,1uH+/-10%,1.3A,non-shd
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Bourns 3116
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AUD 0.0947
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Wirewound Semi - Shielded1 uH10 %1.3 A -- 40 C+ 125 C--Standard2.4 mm1.4 mm1.3 mm-Ferrite CWF2414Reel , Cut Tape
B82422A1104J100


RF Inductors - SMD SMT-INDUCTOR 1210 100 UH 5%, AEC-Q200
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TDK 3113
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AUD 0.319
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Wirewound1210 (3225 METRIC)Unshielded100 uH5 %65 mA11.5 Ohms-- 55 C+ 145 C277 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
NLV32T-R39J-EF


RF Inductors - SMD 390nH 450mohms 450mA Wound Ferrite
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TDK 3111
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AUD 0.143
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Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded390 nH5 %450 mA450 mOhms-- 40 C+ 105 C30250 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
AISC-1008-5R6J-T


RF Inductors - SMD FIXED IND 5.6UH 240MA 5.7 OHM
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ABRACON 3109
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AUD 0.2902
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Wirewound1008 (2520 METRIC)Unshielded5.6 uH5 %240 mA5.7 Ohms - 40 C+ 125 C2040 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
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