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
  
                         
IMC1210ER2R2J


RF Inductors - SMD 2.2uh 5%
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Vishay 3237
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.6443

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Molded1210 (3225 METRIC)Unshielded2.2 uH5 %320 mA1 Ohms    320 MHzStandard3.2 mm2.49 mm    IMCReel , Cut Tape
LQW18ANR21J8ZD


RF Inductors - SMD
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Murata 3233
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1553

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Wirewound0603 (1608 METRIC)Unshielded210 nH5 %280 mA1.98 Ohms-- 55 C+ 125 C271.33 GHzStandard1.65 mm0.99 mm0.9 mm- AEC - Q200LQWReel , Cut Tape
WCL3225-100-R


RF Inductors - SMD 10 UH 20%
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Eaton 3232
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1595

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Wirewound1210 (3225 METRIC)Unshielded10 uH5 %300 mA1 Ohms-- 40 C+ 85 C1030 MHzStandard3.5 mm2.9 mm2.25 mm-  WCLReel , Cut Tape
LQW18AN20NG0ZD


RF Inductors - SMD
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Murata 3231
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1287

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Wirewound0603 (1608 METRIC)Unshielded20 nH2 %550 mA160 mOhms-- 55 C+ 125 C404.9 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
B82422H1333K


RF Inductors - SMD 33uH 280mA 10% 3.2x2.5mm SMD
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TDK 3229
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AUD 0.3768

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Wirewound1210 (3225 METRIC)Unshielded33 uH10 %280 mA1.5 Ohms340 mA- 55 C+ 150 C1215 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200B82422HReel , Cut Tape
MLF2012A1R0MTD25


RF Inductors - SMD 1.0uH 300mohms 80mA +/-20% Fer AEC-Q200
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TDK 3228
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AUD 0.1656

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Multilayer0805 (2012 METRIC)Shielded1 uH20 %80 mA300 mOhms-- 55 C+ 125 C45160 MHzStandard2 mm1.25 mm0.85 mm-FerriteAEC - Q200MLFReel , Cut Tape
B82422H1153J000


RF Inductors - SMD SMT-INDUCTOR1210H 15 UH 5%, AEC-Q200
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TDK 3227
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.5694

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Wirewound1210 (3225 METRIC)Unshielded15 uH5 %390 mA720 mOhms535 mA- 55 C+ 150 C1226 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200B82422HReel , Cut Tape
B82422A3470J100


RF Inductors - SMD SMT-INDUCTOR 1210 0.047UH 5%, AEC-Q200
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TDK 3224
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AUD 0.319

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Wirewound1210 (3225 METRIC)Unshielded47 nH5 %510 mA190 mOhms-- 55 C+ 145 C261.35 GHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422AReel , Cut Tape
LQW15AN2N2D10D


RF Inductors - SMD 2.2 NH
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Murata 3213
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.088

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Wirewound0402 (1005 METRIC)Unshielded2.2 nH0.5 nH1 A27 mOhms-- 55 C+ 125 C2514 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQG18HN22NJ00D


RF Inductors - SMD 22 NH 5%
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Murata 708
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.04

Multiples of: 10

Multilayer0603 (1608 METRIC)Unshielded22 nH5 %500 mA500 mOhms-- 40 C+ 85 C122.3 GHzStandard1.6 mm0.8 mm0.8 mm-Air LQGReel , Cut Tape
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