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
  
                         
NLV32T-8R2J-EFD


RF Inductors - SMD 8.2uH 2.0ohms 170mA Wound Fer AEC-Q200
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TDK 37722
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between Wed. 19 Nov to Fri. 21 Nov
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AUD 0.1486

Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded8.2 uH5 %170 mA2 Ohms-- 40 C+ 105 C3035 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
LCCI0201S3N9GTAR


RF Inductors - SMD 3.9nH Tol 0.3nH 0201 400mA DCR=.3 Ohms
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Kyocera AVX 37665
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between Wed. 19 Nov to Fri. 21 Nov
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AUD 0.0101

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded3.9 nH0.3 nH400 mA300 mOhms-- 40 C+ 85 C56.5 GHzStandard0.6 mm0.3 mm0.3 mm-  LCCIReel , Cut Tape
LCCI0402J6N8GTAR


RF Inductors - SMD 6.8nH Tol 5% 0402 60 0mA DCR=0.25 Ohms
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Kyocera AVX 37276
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between Wed. 19 Nov to Fri. 21 Nov
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AUD 0.0121

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Multilayer0402 (1005 METRIC)Unshielded6.8 nH5 %600 mA250 mOhms-- 40 C+ 85 C84.5 GHzStandard1 mm0.5 mm0.5 mm-Ceramic LCCIReel , Cut Tape
LQP03HQ1N6W02D


RF Inductors - SMD 1.6 NH .05%
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Murata 37155
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between Wed. 19 Nov to Fri. 21 Nov
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AUD 0.1636

Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded1.6 nH0.05 nH1 A50 mOhms - 55 C+ 125 C2010 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
LCCI0402J8N2GTAR


RF Inductors - SMD 8.2nH Tol 5% 0402 50 0mA DCR=0.28 Ohms
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Kyocera AVX 37022
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between Wed. 19 Nov to Fri. 21 Nov
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AUD 0.0147

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded8.2 nH5 %500 mA280 mOhms-- 40 C+ 85 C83.7 GHzStandard1 mm0.5 mm0.5 mm-Ceramic LCCIReel , Cut Tape
LQP02TN39NH02D


RF Inductors - SMD
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Murata 36827
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between Wed. 19 Nov to Fri. 21 Nov
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AUD 0.0587

Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded39 nH3 %90 mA7 Ohms-- 55 C+ 125 C41.6 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
LQG15HH3N6S02D


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 36624
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between Wed. 19 Nov to Fri. 21 Nov
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AUD 0.0949

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded3.6 nH0.3 nH750 mA140 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LCCI0201B0N5GTAR


RF Inductors - SMD .5nH Tol 0.1nH 0201 850mA DCR=.08 Ohms
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Kyocera AVX 36391
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between Wed. 19 Nov to Fri. 21 Nov
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AUD 0.0101

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded500 pH0.1 nH850 mA70 mOhms-- 40 C+ 85 C410 GHzStandard0.6 mm0.3 mm0.3 mm-  LCCIReel , Cut Tape
LQG15HS5N6S02D


RF Inductors - SMD 5.6 NH +-.3NH
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Murata 35599
Ships to you
between Thu. 27 Nov to Tue. 02 Dec
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AUD 0.0061

Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded5.6 nH0.3 nH650 mA180 mOhms - 55 C+ 125 C84.5 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQW15AN56NG00D


RF Inductors - SMD 56 NH 2%
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Murata 31777
Ships to you
between Thu. 27 Nov to Tue. 02 Dec
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AUD 0.0369

Multiples of: 20

Wirewound0402 (1005 METRIC)Unshielded56 nH2 %200 mA1.17 Ohms-- 55 C+ 125 C252.8 GHzStandard1 mm0.5 mm0.5 mm-  LQWReel , Cut Tape
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