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
  
                         
LQW15AN6N8G8ZD


RF Inductors - SMD 6.8 NH 2%
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Murata 18213
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AUD 0.1106

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Wirewound0402 (1005 METRIC)Shielded6.8 nH2 %1.45 A68 mOhms-- 55 C+ 125 C301.45 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
L04024R7BHNTR


RF Inductors - SMD 4.7nH
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Kyocera AVX 10480
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AUD 0.5613

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Thin Film0402 (1005 METRIC)Unshielded4.7 nH0.1 nH250 mA450 mOhms-- 55 C+ 125 C137.5 GHzStandard1 mm0.58 mm0.35 mm-  L0402Reel , Cut Tape
LQG15HZ18NJ02D


RF Inductors - SMD
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Murata 10474
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between Thu. 09 Jul to Mon. 13 Jul
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AUD 0.0369

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Multilayer0402 (1005 METRIC)Unshielded18 nH5 %400 mA360 mOhms-- 55 C+ 125 C82.2 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQW18ASR12G0ZD


RF Inductors - SMD 120 NH 2%
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Murata 10472
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between Thu. 09 Jul to Mon. 13 Jul
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AUD 0.1056

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Wirewound0603 (1608 METRIC)Unshielded120 nH2 %300 mA650 mOhms-- 40 C+ 125 C321.3 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQW18ANR30G80D


RF Inductors - SMD 300 NH 2% NH
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Murata 10456
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between Thu. 09 Jul to Mon. 13 Jul
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AUD 0.102

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Wirewound0603 (1608 METRIC)Unshielded300 nH2 %220 mA3.12 Ohms-- 55 C+ 125 C251.2 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
LQW18AS9N5J00D


RF Inductors - SMD
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Murata 10454
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between Thu. 09 Jul to Mon. 13 Jul
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AUD 0.0911

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Wirewound0603 (1608 METRIC)Unshielded9.5 nH5 %700 mA135 mOhms-- 40 C+ 125 C285.4 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQW18AN56NG80D


RF Inductors - SMD 56 NH 2%
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Murata 10447
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between Thu. 09 Jul to Mon. 13 Jul
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AUD 0.104

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Wirewound0603 (1608 METRIC)Unshielded56 nH2 %770 mA260 mOhms-- 55 C+ 125 C382.6 GHzStandard1.65 mm0.99 mm0.9 mm-- LQWReel , Cut Tape
LQW2BASR82J00L


820 nH Unshielded Wirewound Inductor 180 mA 2.35Ohm Max 0805 (2015 Metric)
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Murata 9941
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AUD 0.1104

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Wirewound0805 (2015 METRIC)Unshielded820 nH5 %180 mA2.35 Ohms-- 55 C+ 125 C23230 MHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
LQW18ANR22G00D


RF Inductors - SMD .22 UH 2%
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Murata 3408
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between Fri. 03 Jul to Thu. 09 Jul
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AUD 0.0831

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Wirewound0603 (1608 METRIC)Unshielded220 nH2 %120 mA2.5 Ohms-- 55 C+ 125 C251.2 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
MLG1005S7N5JT000


RF Inductors - SMD IND 0402 7.5nH StdQ SMD RF IND
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TDK 562
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AUD 0.0663

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Multilayer0402 (1005 METRIC)Unshielded7.5 nH5 %500 mA250 mOhms-- 55 C+ 125 C84.1 GHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , Cut Tape
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