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
  
                         
MLF1608A1R0JTD25


RF Inductors - SMD 1.0uH 500mohms 50mA +/-5% Fer AEC-Q200
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TDK 5777
Ships to you
between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.1586

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Multilayer0603 (1608 METRIC)Shielded1 uH5 %50 mA500 mOhms-- 55 C+ 125 C35170 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQW03AW14NJ00D


RF Inductors - SMD
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Murata 3007
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.505

Multiples of: 1

Wirewound0201 (0603 METRIC)Unshielded14 nH5 %240 mA530 mOhms-- 55 C+ 125 C376 GHzStandard0.53 mm0.4 mm0.4 mm-  LQWReel , Cut Tape
B82422A1122K100


RF Inductors - SMD SMT-INDUCTOR 1210 1.2UH 10%, AEC-Q200
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TDK 3001
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.3051

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Wirewound1210 (3225 METRIC)Unshielded1.2 uH10 %370 mA370 mOhms-- 55 C+ 145 C20300 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
NLV25T-560J-EF


RF Inductors - SMD 56uH 12.1ohms 75mA Wound Ferrite
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TDK 2997
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.1361

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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded56 uH5 %75 mA12.1 Ohms-- 40 C+ 105 C2016 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
LQW15AN7N8C1ZD


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 2987
Ships to you
between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.1474

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded7.8 nH0.2 nH750 mA58 mOhms-- 55 C+ 125 C306.8 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
0805AS-R68J-01


RF Inductors - SMD 680nH 50 MHz 5% Tol
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Fastron 2985
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.1955

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Wirewound0805 (2012 METRIC)Unshielded680 nH5 %170 mA3.5 Ohms-- 40 C+ 150 C37400 MHzStandard2.3 mm1.8 mm1.6 mm-CeramicAEC - Q2000805ASReel , Cut Tape
LQG15HN1N5B02D


1A 1.5nH 80mO 0402 Inductors (SMD) ROHS
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Murata 2984
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.05

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Multilayer Unshielded1.5 nH30 %1 A80 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQG15WH2N3B02D


RF Inductors - SMD Fixed IND 2.3nH 1000mA POWRTRN
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Murata 2953
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.1431

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Multilayer0402 (1005 METRIC)Unshielded2.3 nH0.1 nH1 A70 mOhms-- 55 C+ 125 C237 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQW18ANR27J0ZD


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 2787
Ships to you
between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.1034

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded270 nH5 %110 mA3.4 Ohms-- 55 C+ 125 C30960 MHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
NLCV32T-1R5M-EF


RF Inductors - SMD 1.5uH 143mohms 830mA Wound Ferrite
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TDK 2638
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between Fri. 24 Jul to Wed. 29 Jul
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AUD 0.0457

Multiples of: 10

Wirewound1210 (3225 METRIC)Unshielded1.5 uH20 %830 mA110 mOhms-- 40 C+ 105 C1080 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFReel , Cut Tape
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