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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Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
LQW15AN4N7G8ZD


RF Inductors - SMD
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Murata 4430
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between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.1172

Multiples of: 1

Wirewound0402 (1005 METRIC)Shielded4.7 nH2 %1.2 A71 mOhms-- 55 C+ 125 C311.2 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LQW18CAR21J00D


RF Inductors - SMD Fixed IND 210nH 1050mA NONAUTO
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Murata 4411
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between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.3137

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Wirewound0603 (1608 METRIC)Unshielded210 nH5 %1.05 A115 mOhms-- 55 C+ 125 C331.15 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQW18AN83NG80D


RF Inductors - SMD
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 4403
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between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.1131

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded83 nH2 %550 mA500 mOhms-- 55 C+ 125 C342.23 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
B82432C1683K000


RF Inductors - SMD SMT-INDUCTOR 1812 68UH 10%, AEC-Q200
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TDK 4402
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between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.7168

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Wirewound1812 (4532 METRIC)Unshielded68 uH10 %190 mA2.8 Ohms-- 55 C+ 150 C3010 MHzStandard4.5 mm3.2 mm3.2 mm-FerriteAEC - Q200B82432CReel , Cut Tape
MCL1608V2-331-R


RF Inductors - SMD 330 NH 5%
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Eaton 4393
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between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.0471

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Multilayer0603 (1608 METRIC)Unshielded330 nH5 %150 mA2.8 Ohms - 40 C+ 85 C   1.6 mm0.8 mm0.8 mm   MCLReel , Cut Tape
MCLA2012V1-1R2-R


RF Inductors - SMD MCLA Auto Chip IND 2012 1.2uH 2 Pads
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Eaton 4390
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between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.0672

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Multilayer0805 (2012 METRIC)Unshielded1.2 uH10 %50 mA400 mOhms-- 40 C+ 125 C3565 MHzStandard2 mm1.2 mm0.9 mm- AEC - Q200MCLAReel , Cut Tape
LQW2BASR27J00L


RF Inductors - SMD 270 NH 5%
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Murata 4388
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between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.1051

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Wirewound0805 (2015 METRIC)Unshielded270 nH5 %350 mA1 Ohms-- 55 C+ 125 C48730 MHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
MLF1608C220KTD25


RF Inductors - SMD 22uH 1.7ohms 2mA +/-10% Fer AEC-Q200
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TDK 4338
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between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.1224

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Multilayer0603 (1608 METRIC)Shielded22 uH10 %2 mA1.7 Ohms-- 55 C+ 125 C2038 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
B82422H1223J000


RF Inductors - SMD SMT-INDUCTOR 1210-H 22 UH 5%, AEC-Q200
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TDK 3182
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between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.3586

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Wirewound1210 (3225 METRIC)Unshielded22 uH5 %340 mA1 Ohms440 mA- 55 C+ 150 C1221 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200B82422HReel , Cut Tape
MLG1005S2N0ST000


RF Inductors - SMD IND 0402 2.0nH StdQ SMD RF IND
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TDK 950
Ships to you
between Thu. 23 Jul to Tue. 28 Jul
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AUD 0.0061

Multiples of: 10

Multilayer0402 (1005 METRIC)Unshielded2 nH0.3 nH900 mA150 mOhms-- 55 C+ 125 C79.3 GHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , Cut Tape
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