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
  
                         
AISC-0805F-1R0G-T


RF Inductors - SMD FIXED IND 1UH 245MA 1.2 OHM SMD
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ABRACON 2115
Ships to you
between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.2457

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded1 uH2 %245 mA1.2 Ohms - 40 C+ 125 C1563 MHzStandard2.29 mm1.73 mm1.55 mm Ferrite AISC - 0805FReel , Cut Tape
LQG15HH4N3S02D


RF Inductors - SMD
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Murata 2114
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between Mon. 08 Dec to Thu. 11 Dec
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AUD 0.0322

Multiples of: 20

Multilayer0402 (1005 METRIC)Unshielded4.3 nH0.3 nH750 mA140 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
CC453232-180KL


RF Inductors - SMD 18uH 10% 2.52MHz
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Bourns 2114
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.2217

Multiples of: 1

Wirewound1812 (4532 METRIC)Unshielded18 uH10 %400 mA800 mOhms-- 40 C+ 125 C1019 MHzStandard4.2 mm3.2 mm3.2 mm-Ferrite CC453232Reel , Cut Tape
LQW18CNR10K0ZD


RF Inductors - SMD Fixed IND 100nH 1000mA INFOTMT
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Murata 2112
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.314

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded100 nH10 %1 A100 mOhms-- 55 C+ 125 C-1.26 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
MLF2012DR68MT000


RF Inductors - SMD 2mm x 1.25mm x 1.25mm, -55 to +125 degC, 150mA, 0.68?H, 600mohm
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TDK 2110
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.0908

Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded680 nH20 %150 mA600 mOhms-- 55 C+ 125 C25190 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
L08053R3DEWTR


RF Inductors - SMD 3.3nH
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Kyocera AVX 2104
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.5896

Multiples of: 1

Thin Film0805 (2012 METRIC)Unshielded3.3 nH0.5 nH1.5 A110 mOhms-- 55 C+ 125 C3810 GHzStandard2.11 mm1.5 mm0.91 mm-  0603, 0805Reel , Cut Tape
MLF1608DR68MTD25


RF Inductors - SMD 680nH 1.25ohms 70mA +/-20% Fer AEC-Q200
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TDK 2100
Ships to you
between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.125

Multiples of: 1

Multilayer0603 (1608 METRIC)Shielded680 nH20 %70 mA1.25 Ohms-- 55 C+ 125 C15210 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQW2UAS68NG00L


RF Inductors - SMD
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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.

Murata 2100
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1666

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded68 nH2 %1 A200 mOhms-- 55 C+ 125 C651.3 GHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
LQW18AN9N9C80D


RF Inductors - SMD
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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.

Murata 2083
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1312

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded9.9 nH0.2 nH1.6 A52 mOhms-- 55 C+ 125 C384.75 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
LQW2UASR33F00L


RF Inductors - SMD 330 NH 1%
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Murata 2076
Ships to you
between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.3715

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded330 nH1 %450 mA1.05 Ohms-- 55 C+ 125 C45570 MHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
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