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
  
                         
LQW15AN6N5B0ZD


RF Inductors - SMD
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Murata 5383
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.1352

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Wirewound0402 (1005 METRIC)Unshielded6.5 nH0.1 nH700 mA90 mOhms-- 55 C+ 125 C256 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LQW18ASR18G0CD


RF Inductors - SMD Fixed IND 180nH 240mA NONAUTO
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Murata 5380
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AUD 0.2651

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Wirewound0603 (1608 METRIC)Unshielded180 nH2 %240 mA1.4 Ohms-- 55 C+ 125 C25990 MHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
B82498F3471J


RF Inductors - SMD 470nH 190mA 5% 2.3x1.7mm SMD
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TDK 5370
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AUD 0.3534

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Wirewound0805 (2012 METRIC)Unshielded470 nH5 %190 mA1.9 Ohms-- 55 C+ 125 C30650 MHzStandard2 mm1.3 mm1.4 mm-Ceramic B82498FReel , Cut Tape
LQW18AN11NJ00D


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 5367
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.0724

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Wirewound0603 (1608 METRIC)Unshielded11 nH5 %650 mA110 mOhms-- 55 C+ 125 C356 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
AS0606N0GTR


RF Inductors - SMD 6.0nH 2% SQUARE AIR CORE
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Kyocera AVX 5361
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AUD 0.5758

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Wirewound1.829 mm x 1.397 mm x 1.295 mmUnshielded6 nH2 %2.9 A6 mOhms-- 40 C+ 125 C645.2 GHzStandard1.295 mm1.829 mm1.397 mm-Air ASReel , Cut Tape
MHQ0603P4N7HT000


RF Inductors - SMD IND 0201 4.7nH S-HQ SMD RF IND
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TDK 5354
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AUD 0.0569

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Multilayer0201 (0603 METRIC)Unshielded4.7 nH3 %350 mA400 mOhms-- 55 C+ 125 C167.9 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
LQW2BAS24NJ00L


24 nH Unshielded Wirewound Inductor 500 mA 220mOhm Max 0805 (2015 Metric)
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Murata 5353
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AUD 0.112

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Wirewound0805 (2015 METRIC)Unshielded24 nH5 %500 mA220 mOhms-- 55 C+ 125 C502.4 GHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
LQG15WZ18NG02D


RF Inductors - SMD Fixed IND 18nH 260mA INFOTMT
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Murata 5353
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.1293

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Multilayer0402 (1005 METRIC)Unshielded18 nH2 %260 mA800 mOhms-- 55 C+ 125 C222.3 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LBM2016T6R8J


RF Inductors - SMD 963-LSQMB201616T6R8J RPLCMT PN 0806 6.8uH 1261mOhms 5% 240mA
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Taiyo Yuden 5248
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AUD 0.0983

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Wirewound0806 (2016 METRIC)Unshielded6.8 uH5 %240 mA1.26 Ohms-- 40 C+ 105 C2533 MHzStandard2 mm1.6 mm1.8 mm-  LBMReel , Cut Tape
IMC0603ER33NJ01


RF Inductors - SMD .033uh 5%
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Vishay 4801
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.1509

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Wirewound0603 (1608 METRIC) 33 nH  15 mOhms - 40 C+ 125 C  Standard1.6 mm1.05 mm1.05 mm Ceramic IMCReel , Cut Tape
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