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
  
                         
LQG15HZ9N1H02D


RF Inductors - SMD
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Murata 9621
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between Thu. 09 Jul to Mon. 13 Jul
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AUD 0.0485

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Multilayer0402 (1005 METRIC)Unshielded9.1 nH3 %500 mA260 mOhms-- 55 C+ 125 C83.4 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
PM1210-3R9J-RC


RF Inductors - SMD 3.9uH 5%
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Bourns 9618
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AUD 0.2665

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Wirewound1210 (3225 METRIC)Unshielded3.9 uH5 %250 mA1.3 Ohms-- 55 C+ 105 C3055 MHzStandard2.9 mm2.5 mm2.2 mm-Ferrite PM1210Reel , Cut Tape
LQW15AN47NH0ZD


RF Inductors - SMD
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Murata 9617
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AUD 0.1003

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Wirewound0402 (1005 METRIC)Unshielded47 nH3 %210 mA1.08 Ohms-- 55 C+ 125 C252.9 GHzStandard1 mm0.5 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LQG15WH2N5C02D


RF Inductors - SMD Fixed IND 2.5nH 900mA POWRTRN
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Murata 9615
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AUD 0.071

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Multilayer0402 (1005 METRIC)Unshielded2.5 nH0.2 nH900 mA70 mOhms-- 55 C+ 125 C236.5 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
MHQ1005PR27GT000


RF Inductors - SMD IND 0402 270nH S-HQ SMD RF IND
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TDK 9614
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AUD 0.0963

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Multilayer0402 (1005 METRIC)Unshielded270 nH2 %80 mA7 Ohms-- 55 C+ 125 C18900 MHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
LQW15AN3N2D0ZD


RF Inductors - SMD
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Murata 9612
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AUD 0.1131

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Wirewound0402 (1005 METRIC)Unshielded3.2 nH0.5 nH500 mA170 mOhms-- 55 C+ 125 C1514 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LQW15AN9N0J80D


RF Inductors - SMD
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Murata 9610
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AUD 0.1057

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Wirewound0402 (1005 METRIC)Unshielded9 nH5 %1.42 A70 mOhms-- 55 C+ 125 C306.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
MLG1005SR30JTD25


RF Inductors - SMD IND 0402 300nH StdQ AEC Q200 RF IND
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TDK 9608
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AUD 0.0732

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Multilayer0402 (1005 METRIC)Unshielded300 nH5 %50 mA6.5 Ohms-- 55 C+ 125 C6400 MHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
MLG1005S0N9CTD25


RF Inductors - SMD IND 0402 0.9nH StdQ AEC Q200 RF IND
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TDK 9607
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AUD 0.0908

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Multilayer0402 (1005 METRIC)Unshielded900 pH0.2 nH1 A100 mOhms-- 55 C+ 125 C-17.7 GHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
CW100505-3N3J


RF Inductors - SMD 3.3nH 5% 250 MHz 0.066ohms
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Bourns 9607
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AUD 0.1749

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Wirewound0402 (1005 METRIC)Unshielded3.3 nH5 %840 mA66 mOhms-- 55 C+ 125 C206 GHzStandard1 mm0.55 mm0.5 mm-Ceramic CW100505Reel
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