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
  
                         
LQW2BASR18G00L


RF Inductors - SMD .18 UH 2%
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Murata 20779
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AUD 0.127
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Wirewound0805 (2015 METRIC)Unshielded180 nH2 %400 mA640 mOhms-- 55 C+ 125 C50920 MHzStandard2.09 mm1.53 mm1.42 mm-  LQW2BAReel , Cut Tape
MHQ0402PSA4N7HT000


RF Inductors - SMD 01005, 4.7nH +-3% S-HQ SMD RF IND
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TDK 20711
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AUD 0.0396
Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded4.7 nH3 %200 mA800 mOhms-- 55 C+ 125 C108.14 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
MLG0603P39NHT000


RF Inductors - SMD IND 0201 39nH Hi-Q SMD RF IND
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TDK 20651
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AUD 0.0248
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Multilayer0201 (0603 METRIC)Unshielded39 nH3 %120 mA2.4 Ohms-- 55 C+ 125 C102.2 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
LQP03TQ1N5W02D


RF Inductors - SMD 1.5nH 650mA 0201 (0603 metric) SUGGESTED ALT LQP03HQ1N5W02D
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Murata 20594
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AUD 0.0379
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded1.5 nH0.05 nH650 mA100 mOhms-- 55 C+ 125 C1715 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
MLF2012DR47KT000


200mA 470nH ±10% 250mO 0805 Inductors (SMD) ROHS
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TDK 20554
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AUD 0.0941
Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded470 nH10 %200 mA500 mOhms - 55 C+ 125 C25230 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
LQW18AN18NJ00D


RF Inductors - SMD 18 NH 5%
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Murata 20505
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AUD 0.0498
Multiples of: 10

Wirewound0603 (1608 METRIC)Unshielded18 nH5 %550 mA160 mOhms-- 55 C+ 125 C405.5 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQP03TG2N0C02D


RF Inductors - SMD
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Murata 20409
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AUD 0.0132
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded2 nH0.2 nH450 mA250 mOhms - 55 C+ 125 C1312.5 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQW15AN27NG80D


RF Inductors - SMD 27 NH 2%
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Murata 20370
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AUD 0.0873
Multiples of: 10

Wirewound0402 (1005 METRIC)Unshielded27 nH2 %680 mA288 mOhms-- 55 C+ 125 C304 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
AIML-1206-4R7K-T


RF Inductors - SMD FIXED IND 4.7UH 50MA 700 MOHM
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ABRACON 20370
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AUD 0.1594
Multiples of: 3000

Multilayer Ferrite Chip Inductor1206 (3216 METRIC)Shielded4.7 uH10 %50 mA700 mOhms - 55 C+ 125 C5041 MHzStandard3.2 mm1.6 mm1.1 mm Ferrite AIML - 1206Reel , Cut Tape
AIML-1206-R047M-T


RF Inductors - SMD FIXED IND 47NH 300MA 150 MOHM
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ABRACON 20370
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AUD 0.18
Multiples of: 3000

Multilayer Ferrite Chip Inductor1206 (3216 METRIC)Shielded47 nH20 %300 mA150 mOhms - 55 C+ 125 C30400 MHzStandard3.2 mm1.6 mm1.1 mm Ferrite AIML - 1206Reel , Cut Tape
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