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
  
                         
LQW15AN56NG0ZD


RF Inductors - SMD
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Murata 19361
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.115

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Wirewound0402 (1005 METRIC)Unshielded56 nH2 %200 mA1.17 Ohms-- 55 C+ 125 C252.8 GHzStandard1 mm0.5 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LQP02HQ1N2B02L


RF Inductors - SMD
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Murata 19360
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between Fri. 28 Nov to Wed. 03 Dec
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AUD 0.0101

Multiples of: 20

Thin Film01005 (0402 METRIC)Unshielded1.2 nH0.1 nH800 mA60 mOhms-- 55 C+ 125 C1415 GHzStandard0.4 mm0.2 mm0.3 mm-  LQPReel , Cut Tape
LQG15WH1N0B02D


RF Inductors - SMD 1 NH 1200MA
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Murata 19360
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.1595

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded1 nH0.1 nH1.2 A30 mOhms-- 55 C+ 125 C-15 GHzStandard1 mm0.6 mm0.5 mm-Air LQGReel , Cut Tape
LBM2016TR47J


RF Inductors - SMD 963-LSQMB201616TR47J RPLCMT PN 0806 .47uH 338mOhms 5% 430mA
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Taiyo Yuden 19355
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AUD 0.0929

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Wirewound0806 (2016 METRIC)Unshielded470 nH5 %430 mA338 mOhms-- 40 C+ 105 C30350 MHzStandard2 mm1.6 mm1.8 mm-  LBMReel , Cut Tape
LQP02TN9N1J02D


RF Inductors - SMD
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Murata 19351
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between Fri. 28 Nov to Wed. 03 Dec
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AUD 0.0034

Multiples of: 50

Thin Film01005 (0402 METRIC)Unshielded9.1 nH5 %140 mA2.1 Ohms-- 55 C+ 125 C84 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
LQP02TN33NH02D


RF Inductors - SMD
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Murata 19351
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between Fri. 28 Nov to Wed. 03 Dec
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AUD 0.0142

Multiples of: 50

Thin Film01005 (0402 METRIC)Unshielded33 nH3 %90 mA6.5 Ohms-- 55 C+ 125 C41.8 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
MHQ0402PSA1N3CT000


RF Inductors - SMD 01005, 1.3nH +-0.2nH S-HQ SMD RF IND
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TDK 19351
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AUD 0.0525

Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded1.3 nH0.2 nH400 mA200 mOhms-- 55 C+ 125 C1016.61 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQP02TQ3N4B02D


HF Inductors 3.4nH ±0.1nH 280mA 01005 RoHS
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Murata 19351
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AUD 0.0917

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Thin Film01005 (0402 METRIC)Unshielded3.4 nH0.1 nH280 mA1 Ohms-- 55 C+ 125 C109.7 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
MHQ0402PSA2N0ST000


RF Inductors - SMD 01005, 2.0nH +-0.3nH S-HQ SMD RF IND
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TDK 19341
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AUD 0.0525

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Multilayer01005 (0402 METRIC)Unshielded2 nH0.3 nH400 mA400 mOhms-- 55 C+ 125 C1012.76 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
MHQ0402PSA1N7CT000


RF Inductors - SMD 01005, 1.7nH +-0.2nH S-HQ SMD RF IND
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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.

TDK 19341
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AUD 0.0525

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Multilayer01005 (0402 METRIC)Unshielded1.7 nH0.2 nH400 mA400 mOhms-- 55 C+ 125 C1014.22 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
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