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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(Ex. GST)(▲▼)		Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
NLCV32T-150K-EF


RF Inductors - SMD 15uH 728mohms 370mA Wound Ferrite
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TDK 7003
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AUD 0.0635
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Wirewound1210 (3225 METRIC)Unshielded15 uH10 %370 mA560 mOhms-- 40 C+ 105 C1526 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFReel , Cut Tape
CW201212-27NJ


RF Inductors - SMD 27 NH 5% WIREWOUND
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Bourns 4357
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AUD 0.1913
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Wirewound0805 (2012 METRIC)Unshielded27 nH5 %600 mA120 mOhms-- 40 C+ 125 C602.6 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW201212Reel , Cut Tape
LQW15AN3N1D00D


RF Inductors - SMD
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Murata 4356
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AUD 0.0929
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Wirewound0402 (1005 METRIC)Unshielded3.1 nH0.5 nH570 mA130 mOhms-- 55 C+ 125 C2014 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
L0201R56AHSTR


RF Inductors - SMD 0.56nH
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Kyocera AVX 4355
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AUD 0.1948
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Thin Film0201 (0603 METRIC)Unshielded560 pH0.05 nH500 mA100 mOhms-- 55 C+ 125 C931 GHzStandard0.6 mm0.325 mm0.225 mm-  Accu - LReel , Cut Tape
AS0812N1JTR


RF Inductors - SMD 12.1nH 5% Square Air Core
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Kyocera AVX 4355
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AUD 0.4516
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Wirewound2.134 mm x 1.829 mm x 1.854 mmUnshielded12.1 nH5 %4.4 A7 mOhms-- 40 C+ 125 C1304.3 GHzStandard1.854 mm2.134 mm1.829 mm-Air ASReel , Cut Tape
AIML-0603-R12K-T


RF Inductors - SMD FIXED IND 120NH 50MA 500 MOHM
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ABRACON 4352
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AUD 0.0465
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Multilayer0603 (1608 METRIC)Shielded120 nH10 %50 mA500 mOhms - 55 C+ 125 C15350 MHzStandard1.6 mm0.8 mm0.8 mm Ferrite AIML - 0603Reel , Cut Tape
LQW15AN8N2J8ZD


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 4337
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AUD 0.1051
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded8.2 nH5 %1.5 A69 mOhms - 55 C+ 125 C326.5 GHzStandard1 mm0.6 mm0.5 mm  AEC - Q200LQWReel , Cut Tape
LQW18ANR18J8ZD


RF Inductors - SMD
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Murata 4021
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AUD 0.1293
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Wirewound0603 (1608 METRIC)Unshielded180 nH5 %310 mA1.65 Ohms-- 55 C+ 125 C251.38 GHzStandard1.65 mm0.99 mm0.9 mm- AEC - Q200LQWReel , Cut Tape
MLF2012A1R5JT000


RF Inductors - SMD 2mm x 1.25mm x 0.85mm, -55 to +125 degC, 80mA, 1.5?H, 400mohm
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TDK 3360
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AUD 0.1034
Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded1.5 uH5 %80 mA400 mOhms-- 55 C+ 125 C45140 MHzStandard2 mm1.25 mm0.85 mm-Ferrite MLFReel , Cut Tape
LQW18AN30NG00D


RF Inductors - SMD 30 NH 2%
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Murata 2231
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AUD 0.0495
Multiples of: 10

Wirewound0603 (1608 METRIC)Unshielded30 nH2 %420 mA230 mOhms-- 55 C+ 125 C403.3 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
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