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
  
                         
LQW18AN36NJ0ZD


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 4073
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1293

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Wirewound0603 (1608 METRIC)Unshielded36 nH5 %400 mA260 mOhms-- 55 C+ 125 C402.9 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
MLF1608A4R7KTD25


RF Inductors - SMD 4.7uH 1.6ohms 30mA +/-10% Fer AEC-Q200
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TDK 4073
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1521

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Multilayer0603 (1608 METRIC)Shielded4.7 uH10 %30 mA1.6 Ohms-- 55 C+ 125 C3580 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
MLG0603S30NJT000


RF Inductors - SMD IND 0201 30nH StdQ SMD RF IND
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TDK 4072
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AUD 0.0341

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Multilayer0201 (0603 METRIC)Unshielded30 nH5 %100 mA1.6 Ohms-- 55 C+ 125 C62 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLGReel , Cut Tape
LQG15WH3N6B02D


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 4065
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1757

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Multilayer0402 (1005 METRIC)Unshielded3.6 nH0.1 nH900 mA90 mOhms-- 55 C+ 125 C235.5 GHzStandard1 mm0.6 mm0.5 mm-Air LQGReel , Cut Tape
LQW18ANR39J80D


RF Inductors - SMD
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Murata 4064
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1118

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded390 nH5 %190 mA4.23 Ohms-- 55 C+ 125 C251.1 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
LQW18ANR20J0ZD


RF Inductors - SMD
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Murata 4061
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1212

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Wirewound0603 (1608 METRIC)Unshielded200 nH5 %120 mA2.4 Ohms-- 55 C+ 125 C251.25 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQW2BASR27J00L


RF Inductors - SMD 270 NH 5%
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Murata 4060
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1173

Multiples of: 1

Wirewound0805 (2015 METRIC)Unshielded270 nH5 %350 mA1 Ohms-- 55 C+ 125 C48730 MHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
LQG15WH24NJ02D


RF Inductors - SMD Fixed IND 24nH 230mA POWRTRN
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Murata 4055
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0688

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded24 nH5 %230 mA1.2 Ohms-- 55 C+ 125 C202 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
HLQ022R4BTTR


RF Inductors - SMD 2.4nH
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Kyocera AVX 4054
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3295

Multiples of: 1

Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded2.4 nH0.1 nH245 mA200 mOhms-- 55 C+ 125 C177 GHzStandard1 mm0.58 mm0.35 mm-  HLQReel , Cut Tape
MLF1608C150KTA00


2mA 15uH ±10% 800mO 0603 Inductors (SMD) ROHS
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TDK 3986
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0475

Multiples of: 10

Multilayer0603 (1608 METRIC)Shielded15 uH10 %2 mA1.5 Ohms-- 55 C+ 125 C2042 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
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