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
  
                         
LQW15AN1N5C8ZD


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 10024
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between Thu. 09 Jul to Mon. 13 Jul
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AUD 0.1131

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Wirewound0402 (1005 METRIC)Unshielded1.5 nH0.2 nH2.1 A28 mOhms-- 55 C+ 125 C2018 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQW18ANR22J0ZD


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 10012
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between Thu. 09 Jul to Mon. 13 Jul
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AUD 0.0944

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Wirewound0603 (1608 METRIC)Unshielded220 nH5 %120 mA2.5 Ohms-- 55 C+ 125 C251.2 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQW15AN6N5C00D


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 10000
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between Thu. 09 Jul to Mon. 13 Jul
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AUD 0.0707

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Wirewound0402 (1005 METRIC)Unshielded6.5 nH0.2 nH700 mA90 mOhms - 55 C+ 125 C256 GHzStandard1 mm0.6 mm0.5 mm   LQWReel , Cut Tape
KLZ1608AHR1R0WTD25


RF Inductors - SMD 1uH 10MHz 20% 1608 AEC-Q200
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TDK 9981
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AUD 0.1203

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Multilayer0603 (1608 METRIC)Shielded1 uH20 %600 mA150 mOhms190 mA- 55 C+ 150 C--Flexible (Soft)1.6 mm0.8 mm0.95 mm-FerriteAEC - Q200KLZ - HRReel , Cut Tape
B82496C3151J


RF Inductors - SMD 150nH 130mA 5.0ohms
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TDK 9980
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AUD 0.2599

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Wirewound0603 (1608 METRIC)Unshielded150 nH5 %130 mA5 Ohms-- 55 C+ 150 C51.6 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200SIMID - CReel , Cut Tape
MLJ1608WR10JT000


RF Inductors - SMD 0.1uH 5% 0.13ohms 700mA
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TDK 9898
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AUD 0.1383

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NFC Inductor0603 (1608 METRIC)Shielded100 nH5 %800 mA130 mOhms900 mA- 55 C+ 125 C15600 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLJReel , Cut Tape
MHQ1005PR33GT000


RF Inductors - SMD IND 0402 330nH S-HQ SMD RF IND
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TDK 9501
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AUD 0.1072

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Multilayer0402 (1005 METRIC)Unshielded330 nH2 %80 mA8.2 Ohms-- 55 C+ 125 C13670 MHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
LQG15HH1N8S02D


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 9054
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between Thu. 09 Jul to Mon. 13 Jul
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AUD 0.0833

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Multilayer0402 (1005 METRIC)Unshielded1.8 nH0.3 nH950 mA80 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQG15HZ6N8H02D


600mA 6.8nH ±3% 220mO 0402 Inductors (SMD) ROHS
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Murata 8929
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between Thu. 09 Jul to Mon. 13 Jul
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AUD 0.0429

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Multilayer0402 (1005 METRIC)Unshielded6.8 nH3 %600 mA220 mOhms - 55 C+ 125 C84.5 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
PE-0402CL4N7STT


RF Inductors - SMD 0402 4.7nH 300mA DCR=200mOhms RF
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Pulse 0
6 to 16 Weeks Calender.png

AUD 0.0264

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Multilayer0402 (1005 METRIC)Unshielded4.7 nH0.3 nH300 mA200 mOhms-- 55 C+ 125 C84 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
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