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
  
                         
7447840030G


RF Inductors - SMD WE-MK 0.3A 3nH Shiel 0402 DCR=180 mOhms
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Wurth 4850
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AUD 0.0432

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Multilayer0402 (1005 METRIC)Shielded3 nH0.1 nH300 mA180 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Ceramic WE - MKReel , Cut Tape
7447840147G


RF Inductors - SMD WE-MK 0.2A 47nH Shld 0402 DCR=1.15 Ohms
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Wurth 4850
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AUD 0.0432

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Multilayer0402 (1005 METRIC)Shielded47 nH2 %200 mA1.15 Ohms-- 55 C+ 125 C81 GHzStandard1 mm0.5 mm0.5 mm-Ceramic WE - MKReel , Cut Tape
7847806150


RF Inductors - SMD WE-MCI 15nH 0.32 Ohms Q-Factor=12 AEC-Q200
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Wurth 4850
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by Mon. 17 Nov
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AUD 0.0432

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Multilayer0603 (1608 METRIC)Shielded15 nH5 %300 mA320 mOhms-- 55 C+ 125 C122.3 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200WE - MCIReel , Cut Tape
7847806820


RF Inductors - SMD WE-MCI 82nH 0.95 Ohms Q-Factor=12 AEC-Q200
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Wurth 4850
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AUD 0.0432

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Multilayer0603 (1608 METRIC)Shielded82 nH5 %300 mA950 mOhms-- 55 C+ 125 C12600 MHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200WE - MCIReel , Cut Tape
7447840015G


RF Inductors - SMD WE-MK 0.3A 1.5nH Shd 0402 DCR=100 mOhms
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Wurth 4850
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AUD 0.0432

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Multilayer0402 (1005 METRIC)Shielded1.5 nH0.1 nH300 mA100 mOhms-- 55 C+ 125 C88 GHzStandard1 mm0.5 mm0.5 mm-Ceramic WE - MKReel , Cut Tape
7847805820


RF Inductors - SMD WE-MCI 8.2nH 0.24 Ohms Q-Factor=10 AEC-Q200
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Wurth 4850
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AUD 0.0432

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Multilayer0603 (1608 METRIC)Shielded8.2 nH5 %300 mA240 mOhms-- 55 C+ 125 C103.5 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200WE - MCIReel , Cut Tape
7447840122G


RF Inductors - SMD WE-MK 0.3A 22nH Shld 0402 DCR=580 mOhms
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Wurth 4850
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AUD 0.0432

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Multilayer0402 (1005 METRIC)Shielded22 nH2 %300 mA580 mOhms-- 55 C+ 125 C81.8 GHzStandard1 mm0.5 mm0.5 mm-Ceramic WE - MKReel , Cut Tape
7447840127G


RF Inductors - SMD WE-MK 0.3A 27nH Shld 0402 DCR=670 mOhms
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Wurth 4850
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AUD 0.0432

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Multilayer0402 (1005 METRIC)Shielded27 nH2 %300 mA670 mOhms-- 55 C+ 125 C81.6 GHzStandard1 mm0.5 mm0.5 mm-Ceramic WE - MKReel , Cut Tape
7447840118G


RF Inductors - SMD WE-MK DCRes=0.51Ohms 0402 0.3A +/- 2%
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Wurth 4850
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AUD 0.0432

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Multilayer0402 (1005 METRIC)Shielded18 nH2 %300 mA510 mOhms-- 55 C+ 125 C82.1 GHzStandard1 mm0.5 mm0.5 mm-Ceramic WE - MKReel , Cut Tape
7847806120


RF Inductors - SMD WE-MCI 12nH 0.28 Ohms Q-Factor=12 AEC-Q200
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Wurth 4850
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AUD 0.0432

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Multilayer0603 (1608 METRIC)Shielded12 nH5 %300 mA280 mOhms-- 55 C+ 125 C122.6 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200WE - MCIReel , Cut Tape
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