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
  
                         
LQW15AN6N1G80D


RF Inductors - SMD
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Murata 7143
Ships to you
between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.1276

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded6.1 nH2 %1.6 A56 mOhms - 55 C+ 125 C328 GHzStandard1 mm0.6 mm0.5 mm   LQWReel , Cut Tape
MCQ1V3216-R082-R


RF Inductors - SMD Multi H Q, IND 82nH Q30 300mA 2PADS SMT
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Eaton 7127
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.044

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Multilayer1206 (3216 METRIC)Unshielded82 nH10 %300 mA250 mOhms-- 40 C+ 85 C30280 MHzStandard3.2 mm1.6 mm0.9 mm-  MCQ1VReel , Cut Tape
MHQ1005P56NGTD25


RF Inductors - SMD IND 0402 56nH S-HQ AEC Q200 RF IND
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TDK 7123
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.1918

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Multilayer0402 (1005 METRIC)Unshielded56 nH2 %180 mA1.8 Ohms-- 55 C+ 125 C221.8 GHzStandard1 mm0.5 mm0.6 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
LQW2BAS10NJ00L


10 nH Unshielded Wirewound Inductor 600 mA 100mOhm Max 0805 (2015 Metric)
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Murata 7119
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.1017

Multiples of: 1

Wirewound0805 (2015 METRIC)Unshielded10 nH5 %600 mA100 mOhms-- 55 C+ 125 C604.3 GHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
LQW18AS27NJ00D


RF Inductors - SMD
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Murata 7117
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.0969

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded27 nH5 %600 mA220 mOhms-- 40 C+ 125 C402.8 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQW18AN27NJ80D


RF Inductors - SMD
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Murata 7112
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.1155

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded27 nH5 %1.2 A98 mOhms-- 55 C+ 125 C403.6 GHzStandard1.65 mm0.99 mm0.9 mm-- LQWReel , Cut Tape
LQW15AN16NG0ZD


RF Inductors - SMD
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Murata 7107
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.1352

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded16 nH2 %370 mA240 mOhms-- 55 C+ 125 C254.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
MLG1005S13NHT000


RF Inductors - SMD IND 0402 13nH StdQ SMD RF IND
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TDK 7105
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.0686

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded13 nH3 %400 mA500 mOhms-- 55 C+ 125 C82.9 GHzStandard1 mm0.5 mm0.55 mm-Ceramic MLGReel , Cut Tape
CS160808-82NK


RF Inductors - SMD 0.082uH '10%
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Bourns 7104
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.0733

Multiples of: 1

Multilayer0603 (1608 METRIC)Shielded82 nH10 %200 mA250 mOhms-- 55 C+ 125 C45260 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite  Reel , Cut Tape
LCWC0603GR10GTAR


RF Inductors - SMD 100nH 2%
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Kyocera AVX 7101
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between Tue. 24 Feb to Thu. 26 Feb
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AUD 0.2585

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Wirewound0603 (1608 METRIC)Unshielded100 nH2 %400 mA580 mOhms-- 40 C+ 125 C341.4 GHzStandard1.8 mm1.12 mm1.02 mm-Ceramic LCWCReel , Cut Tape
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