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
  
                         
7447602680A


RF Inductors - SMD WE-KI DCResi=1.2Ohms 680nH 0.4A AEC-Q200
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Wurth 4850
Ships to you
by Mon. 17 Nov
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AUD 0.3171

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded680 nH5 %400 mA1.2 Ohms-- 40 C+ 125 C15188 MHzStandard2 mm1.25 mm1.2 mm-Ceramic WE - KIReel , Cut Tape
7447603180A


RF Inductors - SMD WE-KI DCRes=6.26Ohms 1800nH 0.14A AEC-Q200
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Wurth 4850
Ships to you
by Mon. 17 Nov
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AUD 0.3171

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded1.8 uH5 %140 mA6.26 Ohms-- 40 C+ 125 C18210 MHzStandard2 mm1.25 mm1.2 mm-Ceramic WE - KIReel , Cut Tape
7447603100A


RF Inductors - SMD WE-KI DCResi=2.8Ohms 1000nH 0.18A AEC-Q200
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Wurth 4850
Ships to you
by Mon. 17 Nov
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AUD 0.3171

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded1 uH5 %180 mA2.8 Ohms-- 40 C+ 125 C20250 MHzStandard2 mm1.25 mm1.2 mm-Ceramic WE - KIReel , Cut Tape
HLQ021R6BTTR


RF Inductors - SMD 1.6nH
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Kyocera AVX 4850
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between Fri. 21 Nov to Thu. 27 Nov
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AUD 0.3333

Multiples of: 1

Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded1.6 nH0.1 nH300 mA150 mOhms-- 55 C+ 125 C177 GHzStandard1 mm0.58 mm0.35 mm-  HLQReel
744762233A


RF Inductors - SMD WE-KI 1008 330nH 500mA DCR=900mOhms 5% AEC-Q200
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Wurth 4850
Ships to you
by Mon. 17 Nov
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AUD 0.3413

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded330 nH5 %500 mA900 mOhms-- 40 C+ 125 C45570 MHzStandard2.5 mm2 mm1.6 mm-CeramicAEC - Q200WE - KIReel , Cut Tape
744758327A


RF Inductors - SMD WE-RFH SMD 1008A 2.7uH 520mA 1.1Ohm
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Wurth 4850
Ships to you
by Mon. 17 Nov
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AUD 0.3508

Multiples of: 1

Wirewound Unshielded2.7 uH5 %520 mA1.1 Ohms-- 40 C+ 85 C20135 MHzStandard2.6 mm2.1 mm1.7 mm-Ferrite WE - RFHReel , Cut Tape
HLQ022R0BTTR


RF Inductors - SMD 2.0nH
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Kyocera AVX 4850
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3556

Multiples of: 1

Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded2 nH0.1 nH245 mA180 mOhms-- 55 C+ 125 C177 GHzStandard1 mm0.58 mm0.35 mm-  HLQReel , Cut Tape
7447918


RF Inductors - SMD WE-MI Mulitlayer Ind 10 uH 25 mA 0.6 ohms
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Wurth 4850
Ships to you
by Mon. 17 Nov
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AUD 0.3562

Multiples of: 1

Multilayer1206 (3216 METRIC)Unshielded10 uH10 %25 mA600 mOhms-- 55 C+ 125 C5026 MHzStandard3.2 mm1.6 mm1.1 mm-  WE - MIReel , Cut Tape
744765143A


RF Inductors - SMD WE-KI 0402 43nH 100mA DCR=810mOhms 5% AEC-Q200
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Wurth 4850
Ships to you
by Mon. 17 Nov
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AUD 0.367

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded43 nH5 %100 mA810 mOhms-- 40 C+ 125 C252.03 GHzStandard1 mm0.55 mm0.5 mm-CeramicAEC - Q200WE - KIReel , Cut Tape
HLQ02220HTTR


RF Inductors - SMD 22nH 3%
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Kyocera AVX 4850
Ships to you
between Fri. 21 Nov to Thu. 27 Nov
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AUD 0.3718

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
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