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
  
                         
LQG15WZ2N0C02D


RF Inductors - SMD
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Murata 17052
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between Wed. 08 Jul to Fri. 10 Jul
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AUD 0.0868

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Multilayer0402 (1005 METRIC)Unshielded2 nH0.2 nH1 A50 mOhms-- 55 C+ 125 C238 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQW18AS82NG0CD


RF Inductors - SMD 82 NH 2%
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Murata 17050
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AUD 0.2706

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Wirewound0603 (1608 METRIC)Unshielded82 nH2 %400 mA540 mOhms-- 55 C+ 125 C341.7 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
MHQ1005P1N3ST000


RF Inductors - SMD IND 0402 1.3nH S-HQ SMD RF IND
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TDK 17009
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AUD 0.101

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Multilayer0402 (1005 METRIC)Unshielded1.3 nH0.3 nH1.2 A30 mOhms-- 55 C+ 125 C-20 GHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
MLG0402Q27NHT000


RF Inductors - SMD
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TDK 17004
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AUD 0.0283

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 01005 (0402 METRIC)Unshielded27 nH3 %120 mA3.5 Ohms - 55 C+ 125 C32.5 GHzStandard0.4 mm0.2 mm0.22 mm Ceramic MLG - QReel , Cut Tape
LQG15WH10NJ02D


RF Inductors - SMD
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Murata 16991
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AUD 0.066

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Multilayer0402 (1005 METRIC)Unshielded10 nH5 %500 mA190 mOhms-- 55 C+ 125 C233.3 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
PE-0402CL180JTT


RF Inductors - SMD 0402 18nH 300mA DCR=500mOhms RF
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Pulse 16988
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AUD 0.0264

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Multilayer0402 (1005 METRIC)Unshielded18 nH5 %300 mA500 mOhms-- 55 C+ 125 C82.1 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
MHQ0402PSA0N6BT000


RF Inductors - SMD 01005, 0.6nH +-0.1nH S-HQ SMD RF IND
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TDK 16975
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AUD 0.0357

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Multilayer01005 (0402 METRIC)Unshielded600 pH0.1 nH600 mA150 mOhms-- 55 C+ 125 C-20 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQP03HQ2N2W02D


RF Inductors - SMD
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Murata 16949
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AUD 0.1241

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Thin Film0201 (0603 METRIC)Unshielded2.2 nH0.05 nH600 mA120 mOhms-- 55 C+ 125 C209 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
LQW15AN8N2G0ZD


RF Inductors - SMD
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Murata 15805
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AUD 0.1036

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Wirewound0402 (1005 METRIC)Unshielded8.2 nH2 %540 mA140 mOhms-- 55 C+ 125 C255.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
PM1210-101J-RC


Inductor RF Molded Bobbin Core 100uH 5% 796KHz 20Q-Factor Ferrite 0.04A 11Ohm DCR 1210 T/R
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Bourns 10892
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AUD 0.2208

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Wirewound1210 (3225 METRIC)Unshielded100 uH5 %40 mA11 Ohms-- 55 C+ 105 C2010 MHzStandard2.9 mm2.5 mm2.2 mm-Ferrite PM1210Reel , Cut Tape
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