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
  
                         
LBM2016TR18J


RF Inductors - SMD 963-LSQMB201616TR18J RPLCMT PN 0806 .18uH 195mOhms 5% 560mA
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Taiyo Yuden 1640
Ships to you
between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.0965

Multiples of: 1

Wirewound0806 (2016 METRIC)Unshielded180 nH5 %560 mA195 mOhms-- 40 C+ 105 C30500 MHzStandard2 mm1.6 mm1.8 mm-  LBMReel , Cut Tape
LQW18AS47NG0ZD


RF Inductors - SMD
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Murata 567
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between Wed. 29 Jul to Mon. 03 Aug
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AUD 0.0961

Multiples of: 5

Wirewound0603 (1608 METRIC)Unshielded47 nH2 %600 mA280 mOhms-- 40 C+ 125 C382 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
MHQ0402PSA1N3BT000


RF Inductors - SMD 01005, 1.3nH +-0.1nH S-HQ SMD RF IND
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TDK 556
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.0293

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Multilayer01005 (0402 METRIC)Unshielded1.3 nH0.1 nH400 mA200 mOhms-- 55 C+ 125 C1016.61 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
1812SMS-R10GLC


RF Inductors - SMD 1812 100nH Unshld 2% 1.7A 12.3mOhms AECQ
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Coilcraft 555
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AUD 0.7363

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Wirewound1812 (4532 METRIC)Unshielded100 nH2 %1.7 A12.3 mOhms-- 40 C+ 125 C1001.2 GHzStandard6.35 mm4.95 mm4.2 mm-AirAEC - Q2001812SMSReel , Cut Tape
L04022R7AHNTR


RF Inductors - SMD 2.7nH
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Kyocera AVX 545
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.7241

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Thin Film0402 (1005 METRIC)Unshielded2.7 nH0.05 nH250 mA250 mOhms-- 55 C+ 125 C159.5 GHzStandard1 mm0.58 mm0.35 mm-  L0402Reel , Cut Tape
L06032R7BGWTR


RF Inductors - SMD 2.7nH
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Kyocera AVX 544
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.5947

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Thin Film0603 (1608 METRIC)Unshielded2.7 nH0.1 nH750 mA80 mOhms-- 55 C+ 125 C219 GHzStandard1.6 mm0.81 mm0.61 mm-  0603, 0805Reel , Cut Tape
1812AF-102J-01


1812AF-102J-01
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Fastron 544
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between Wed. 15 Jul to Tue. 21 Jul
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AUD 0.9591

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LQW2BASR15J00L


RF Inductors - SMD .15 UH 5%
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Murata 543
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.112

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Wirewound0805 (2015 METRIC)Unshielded150 nH5 %400 mA560 mOhms-- 55 C+ 125 C50920 MHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
CMH322522-390KL


RF Inductors - SMD 39uH 10% 2.52MHz
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Bourns 540
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.281

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Wirewound1210 (3225 METRIC)Shielded39 uH10 %65 mA6.4 Ohms-- 55 C+ 125 C3015 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite  Reel , Cut Tape
IMC1008ER220J


RF Inductors - SMD 22uH 5%
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Vishay 533
Ships to you
between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.1931

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Wirewound1008 (2520 METRIC)Unshielded22 uH5 %110 mA5 Ohms-- 40 C+ 125 C1522 MHzStandard2.5 mm2 mm1.6 mm-Ferrite IMCReel , Cut Tape
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