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
  
                         
AL01656N0JTS


RF Inductors - SMD 56nH 5% AIR CORE
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Kyocera AVX 1843
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.2423

Multiples of: 1

Wirewound3.81 mm x 4.2 mm x 4.83 mmUnshielded56 nH5 %3 A6.2 mOhms-- 40 C+ 125 C1001.5 GHzStandard4.83 mm3.81 mm4.2 mm-Air ALReel , Cut Tape
AISC-0805-R12G-T


RF Inductors - SMD FIXED IND 120NH 400MA 510 MOHM
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ABRACON 1843
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.2823

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Wirewound0805 (2317 METRIC)Unshielded120 nH2 %400 mA510 mOhms - 40 C+ 125 C501.1 GHzStandard2.29 mm1.73 mm1.55 mm Ceramic AISC - 0805Reel , Cut Tape
LQW2UASR91F00L


RF Inductors - SMD
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Murata 1843
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.3105

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded910 nH1 %380 mA1.68 Ohms-- 55 C+ 125 C35320 MHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
ISC1812ES2R7K


RF Inductors - SMD 2.7uh 10%
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Vishay 1843
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.7048

Multiples of: 1

Molded1812 (4532 METRIC) 2.7 uH  820 mOhms     Standard      ISCReel , Cut Tape
IMC1812ER270J


RF Inductors - SMD 27uh 5%
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Vishay 1843
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.8076

Multiples of: 1

Molded1812 (4532 METRIC) 27 uH  280 mOhms     Standard      IMCReel , Cut Tape
NLV25T-R82J-EF


RF Inductors - SMD 820nH 1.0ohms 260mA Wound Ferrite
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TDK 1841
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1376

Multiples of: 1

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded820 nH5 %260 mA1 Ohms-- 40 C+ 105 C30260 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
0402F-R10K-08


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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Fastron 1838
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.4968

Multiples of: 1

Wirewound1.2 mm x 0.65 mm x 0.7 mmUnshielded100 nH10 %1 A150 mOhms - 40 C+ 85 C 1.4 GHz 1.2 mm0.65 mm0.7 mm FerriteAEC - Q2000402FReel , Cut Tape
IMC1812ES101J


RF Inductors - SMD 100uh 5%
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Vishay 1830
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.5856

Multiples of: 1

Molded1812 (4532 METRIC) 100 uH5 %110 mA8 Ohms - 55 C+ 125 C408 MHzStandard4.5 mm3.2 mm3.2 mm   IMCReel , Cut Tape
MHQ0603P18NJT000


RF Inductors - SMD IND 0201 18nH S-HQ SMD RF IND
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TDK 1829
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.0459

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded18 nH5 %180 mA1.7 Ohms-- 55 C+ 125 C163.7 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
LQP03TN20NH02D


RF Inductors - SMD 20 NH 3%
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Murata 339
Ships to you
between Mon. 08 Dec to Thu. 11 Dec
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AUD 0.0088

Multiples of: 50

Thin Film0201 (0603 METRIC)Unshielded20 nH3 %150 mA2.3 Ohms - 55 C+ 125 C122.2 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
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