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
  
                         
LQG15HHR10H02D


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 5512
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.106

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Multilayer0402 (1005 METRIC)Unshielded100 nH3 %200 mA1.25 Ohms-- 55 C+ 125 C8600 MHzStandard1 mm0.5 mm0.5 mm AirAEC - Q200LQGReel , Cut Tape
LQW18AN4N7B8ZD


RF Inductors - SMD
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Murata 5504
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1412

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Wirewound0603 (1608 METRIC)Unshielded4.7 nH0.1 nH1.5 A54 mOhms-- 55 C+ 125 C2510.4 GHzStandard1.65 mm0.99 mm0.9 mm- AEC - Q200LQWReel , Cut Tape
L08051R5CESTR


RF Inductors - SMD 1.5nH 2000mA 0805 DC =0.05ohm
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Kyocera AVX 5496
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AUD 0.619

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 0805 (2012 METRIC) 1.5 nH               Accu - LReel , Cut Tape
CI160808-56NJ


RF Inductors - SMD 56nH 5% MultiLayer High Frequency
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Bourns 5495
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AUD 0.055

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Multilayer0603 (1608 METRIC)Unshielded56 nH5 %300 mA1 Ohms-- 55 C+ 125 C101.15 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic CI160808Reel , Cut Tape
MHQ1005P1N0CT000


RF Inductors - SMD IND 0402 1.0nH S-HQ SMD RF IND
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TDK 5487
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AUD 0.0985

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Multilayer0402 (1005 METRIC)Unshielded1 nH0.2 nH1.2 A30 mOhms-- 55 C+ 125 C-20 GHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
LQP03HQ1N3C02D


RF Inductors - SMD
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Murata 5480
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0908

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Thin Film0201 (0603 METRIC)Unshielded1.3 nH0.2 nH1.1 A40 mOhms-- 55 C+ 125 C2013 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
NLV32T-4R7J-EFD


RF Inductors - SMD 4.7uH 1.5ohms 220mA Wound Fer AEC-Q200
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TDK 5462
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AUD 0.154

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Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded4.7 uH5 %220 mA1.5 Ohms-- 40 C+ 105 C3050 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
AISC-1008-1R0J-T


RF Inductors - SMD FIXED IND 1UH 370MA 1.8 OHM SMD
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ABRACON 5459
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AUD 0.1632

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Wirewound1008 (2520 METRIC)Unshielded1 uH5 %370 mA1.8 Ohms - 40 C+ 125 C35270 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
LQW18AN4N3B8ZD


RF Inductors - SMD
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Murata 5451
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1696

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded4.3 nH0.1 nH2.1 A36 mOhms-- 55 C+ 125 C3511.6 GHzStandard1.65 mm0.99 mm0.9 mm- AEC - Q200LQWReel , Cut Tape
MLG1005SR16JT000


RF Inductors - SMD IND 0402 160nH StdQ SMD RF IND
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TDK 5445
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0681

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Multilayer0402 (1005 METRIC)Unshielded160 nH5 %150 mA3.8 Ohms-- 55 C+ 125 C8600 MHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , Cut Tape
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