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
  
                         
744901039


RF Inductors - SMD WE-TCI Thinfilm 3.9nH 340mA .5Ohm
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Wurth 4850
Ships to you
by Thu. 02 Jul
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AUD 0.2883

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Thin Film Shielded3.9 nH0.1 nH340 mA500 mOhms-- 40 C+ 125 C136 GHzStandard1 mm0.5 mm0.32 mm-  WE - TCIReel , Cut Tape
HLQ021R6BTTR


RF Inductors - SMD 1.6nH
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Kyocera AVX 4850
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between Wed. 08 Jul to Tue. 14 Jul
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AUD 0.3134

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Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded1.6 nH0.1 nH300 mA150 mOhms-- 55 C+ 125 C177 GHzStandard1 mm0.58 mm0.35 mm-  HLQReel
7447880247


RF Inductors - SMD WE-MK DCResis=2 Ohms 0805 470nH AEC-Q200
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Wurth 4850
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by Thu. 02 Jul
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AUD 0.319

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Multilayer0805 (2012 METRIC)Shielded470 nH5 %300 mA2 Ohms - 55 C+ 125 C10200 MHz 2 mm1.25 mm0.85 mm   WE - MKReel , Cut Tape
744761112A


RF Inductors - SMD WE-KI SMT Wire Wound Ceramic Inductor AEC-Q200
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Wurth 4850
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by Thu. 02 Jul
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AUD 0.3162

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Wirewound                 AEC - Q200WE - KIReel , Cut Tape
7447602C


RF Inductors - SMD WE-KI 0805 100nH 400mA DCR=460mOhms5%
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Wurth 4850
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by Thu. 02 Jul
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AUD 0.3482

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Wirewound0805 (2012 METRIC)Unshielded100 nH5 %400 mA460 mOhms-- 40 C+ 125 C501.2 GHzStandard2.28 mm1.7 mm1.28 mm-Ceramic WE - KIReel , Cut Tape
HLQ02220HTTR


RF Inductors - SMD 22nH 3%
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Kyocera AVX 4850
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between Wed. 08 Jul to Tue. 14 Jul
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AUD 0.3423

Multiples of: 1

Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded22 nH3 %95 mA1.9 Ohms-- 55 C+ 125 C173 GHzStandard1 mm0.58 mm0.35 mm   HLQReel
HLQ02320HTTR


RF Inductors - SMD 32nH 3%
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Kyocera AVX 4850
Ships to you
between Wed. 08 Jul to Tue. 14 Jul
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AUD 0.323

Multiples of: 1

Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded32 nH3 %85 mA2.2 Ohms - 55 C+ 125 C172 GHzStandard1 mm0.58 mm0.35 mm   HLQReel
744760222C


RF Inductors - SMD WE-KI 0805 220nH 400mA DCR=1Ohms 5%
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Wurth 4850
Ships to you
by Thu. 02 Jul
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AUD 0.3563

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded220 nH5 %400 mA1 Ohms-- 40 C+ 125 C35850 MHzStandard2.28 mm1.7 mm1.28 mm-Ceramic WE - KIReel , Cut Tape
744765033A


RF Inductors - SMD WE-KI 0402 3.3nH 840mA DCR=66mOhms 5% AEC-Q200
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Wurth 4850
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by Thu. 02 Jul
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AUD 0.3773

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded3.3 nH5 %840 mA66 mOhms-- 40 C+ 125 C206 GHzStandard1 mm0.55 mm0.5 mm-CeramicAEC - Q200WE - KIReel , Cut Tape
744765130A


RF Inductors - SMD WE-KI 0402 30nH 400mA DCR=300mOhms 5% AEC-Q200
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Wurth 4850
Ships to you
by Thu. 02 Jul
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AUD 0.3854

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Wirewound0402 (1005 METRIC)Unshielded30 nH5 %400 mA300 mOhms-- 40 C+ 125 C252.35 GHzStandard1 mm0.55 mm0.5 mm-CeramicAEC - Q200WE - KIReel , Cut Tape
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