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
  
                         
WCL2520-4R7-R


RF Inductors - SMD WCL Chip IND 2520 4.7uH 2 Pads
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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.

Eaton 3856
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1173

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded4.7 uH5 %210 mA1.72 Ohms-- 40 C+ 85 C1250 MHzStandard2.92 mm2.79 mm2.1 mm-  WCLReel , Cut Tape
ILSB0805ERR27K


RF Inductors - SMD .27uH 10%
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Vishay 3856
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1293

Multiples of: 1

Established Reliability0805 (2012 METRIC)Shielded270 nH10 %250 mA500 mOhms-- 55 C+ 125 C20173 MHzStandard2 mm1.25 mm0.9 mm-  ILSB - 0805Reel , Cut Tape
WCLA1608V1-560-R


RF Inductors - SMD WCLA Auto Chip IND 1608 56nH 2 Pads
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Eaton 3856
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1851

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded56 nH5 %600 mA280 mOhms-- 40 C+ 125 C381.9 GHzStandard1.78 mm1.1 mm0.95 mm- AEC - Q200WCLAReel , Cut Tape
AISC-Q0402HQ-3N3C-T


RF Inductors - SMD IND 3.3nH 1.7A 45m?
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Abracon 3856
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2133

Multiples of: 1

Wirewound0402 (1208 METRIC)Unshielded3.3 nH0.2 nH1.7 A45 mOhms - 40 C+ 125 C9512.8 GHzStandard1.27 mm0.76 mm0.61 mm Ceramic AISC - Q0402HQReel , Cut Tape
PE-0402CL560JTT


RF Inductors - SMD 0402 56nH 200mA DCR=12000mOhms RF
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Pulse 3855
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0293

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded56 nH5 %200 mA1.2 Ohms-- 55 C+ 125 C8750 MHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
WCLA2520V1-3R3-R


RF Inductors - SMD Chip IND 3.3uH 0.715A SMT 2 Pad
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Eaton 3855
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2529

Multiples of: 1

Wirewound1008 (2520 METRIC)Shielded3.3 uH10 %715 mA260 mOhms - 55 C+ 125 C1248 MHz 2.9 mm2.5 mm2.1 mm Ferrite WCLAReel , Cut Tape
B82432C1473J000


RF Inductors - SMD SMT-INDUCTOR 1812 47UH 5%, AEC-Q200
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TDK 3855
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.8177

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Wirewound1812 (4532 METRIC)Unshielded47 uH5 %210 mA2.3 Ohms-- 55 C+ 150 C3012 MHzStandard4.5 mm3.2 mm3.2 mm-FerriteAEC - Q200B82432CReel , Cut Tape
WCLA2520V1-330-R


RF Inductors - SMD Chip IND 33.0uH 0.236A SMT 2 Pad
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Eaton 3854
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2529

Multiples of: 1

Wirewound1008 (2520 METRIC)Shielded33 uH10 %236 mA2.47 mOhms - 55 C+ 125 C1215 MHz 2.9 mm2.5 mm2.1 mm Ferrite WCLAReel , Cut Tape
LQW18CAR40J00D


RF Inductors - SMD Fixed IND 400nH 680mA NONAUTO
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Murata 3852
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3337

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded400 nH5 %680 mA260 mOhms-- 55 C+ 125 C33900 MHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
MLF2012A4R7JT000


RF Inductors - SMD 4.7 UH 5%
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TDK 3821
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0433

Multiples of: 10

Multilayer0805 (2012 METRIC)Shielded4.7 uH5 %30 mA700 mOhms-- 55 C+ 125 C4570 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
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