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
  
                         
MLG0603P4N2CT000


RF Inductors - SMD IND 0201 4.2nH Hi-Q SMD RF IND
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TDK 14065
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between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.0262

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded4.2 nH0.2 nH350 mA400 mOhms-- 55 C+ 125 C146.6 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
MHQ1005P6N8JT000


RF Inductors - SMD IND 0402 6.8nH S-HQ SMD RF IND
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TDK 14057
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between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.1027

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded6.8 nH5 %700 mA140 mOhms-- 55 C+ 125 C235.8 GHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
LQP02HQ39NH02E


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 14055
Ships to you
between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.109

Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded39 nH3 %110 mA3.6 Ohms-- 55 C+ 125 C92.4 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , Cut Tape
MLG0603P8N2JTD25


RF Inductors - SMD IND 0201 8.2nH Hi-Q AEC Q200 RF IND
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TDK 14054
Ships to you
between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.0485

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded8.2 nH5 %250 mA850 mOhms-- 55 C+ 125 C145.2 GHzStandard0.6 mm0.3 mm0.3 mm-CeramicAEC - Q200MLG - PReel , Cut Tape
BSPQ000603040N6B00


RF Inductors - SMD 0.6nH 500MHz 1100mA RDC=0.04mOhms
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Pulse 14051
Ships to you
between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.0702

Multiples of: 1

 0603 (1608 METRIC)Shielded600 pH0.1 nH1.1 A40 mOhms - 55 C+ 125 C2020 GHzStandard0.6 mm0.3 mm0.4 mm Ceramic BSPQReel , Cut Tape
MLG0603S0N4CTD25


RF Inductors - SMD IND 0201 0.4nH StdQ AEC Q200 RF IND
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TDK 14050
Ships to you
between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.0565

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded400 pH0.2 nH600 mA100 mOhms-- 55 C+ 125 C-20 GHzStandard0.6 mm0.3 mm0.3 mm-CeramicAEC - Q200MLGReel , Cut Tape
MLG0603P3N3CT000


RF Inductors - SMD IND 0201 3.3nH Hi-Q SMD RF IND
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TDK 14045
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between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.0293

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded3.3 nH0.2 nH450 mA200 mOhms-- 55 C+ 125 C148.4 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
MHQ0603P4N7HTD25


RF Inductors - SMD 0201 4.7nH Tol 0.1nH AEC-Q200
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TDK 14015
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between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.0852

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded4.7 nH3 %350 mA400 mOhms-- 55 C+ 125 C167.9 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
LQW15AN8N2G80D


RF Inductors - SMD 8.2 NH 2%
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Murata 13793
Ships to you
between Mon. 01 Dec to Thu. 04 Dec
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AUD 0.0871

Multiples of: 10

Wirewound0402 (1005 METRIC)Unshielded8.2 nH2 %1.5 A69 mOhms-- 55 C+ 125 C326.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQP03TQ1N6B02D


RF Inductors - SMD PLEASE SEE MURATA'S SUGGESTED ALTERNATE LQP03HQ1N6B02D
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Murata 0
6 to 16 Weeks Calender.png

AUD 0.0401

Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded1.6 nH0.1 nH650 mA100 mOhms - 55 C+ 125 C1715 GHzStandard0.6 mm0.3 mm0.3 mm Ferrite LQPReel , Cut Tape
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