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
  
                         
CW252016-4R7J


RF Inductors - SMD 4.7 UH 5%
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Bourns 5772
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1742

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded4.7 uH5 %175 mA2.3 Ohms-- 40 C+ 125 C1843 MHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
LQW18AS47NJ0ZD


RF Inductors - SMD
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Murata 5771
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0956

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded47 nH5 %600 mA280 mOhms-- 40 C+ 125 C382 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
5508 181 34 00


RF Inductors - SMD RF Chip Inductor SMD 180nH 0805 5% Tol
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Sumida 5771
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3276

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RF Choke0805 (2012 METRIC)Unshielded180 nH5 %260 mA470 mOhms-- 55 C+ 125 C351.03 GHzStandard2.2 mm1.4 mm1.42 mm-Ceramic 5508Reel , Cut Tape
LQG15WZ1N5S02D


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 5770
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between Fri. 21 Nov to Thu. 27 Nov
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AUD 0.0029

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded1.5 nH0.3 nH1 A40 mOhms-- 55 C+ 125 C2311 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQW15AN7N9C1ZD


RF Inductors - SMD
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Murata 5761
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1474

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded7.9 nH0.2 nH640 mA79 mOhms-- 55 C+ 125 C307.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
B82498F3561J001


RF Inductors - SMD SMT-INDUCTOR 0805 560NH 5%
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TDK 5761
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.448

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded560 nH5 %230 mA1.3 Ohms-- 55 C+ 125 C23400 MHzStandard2 mm1.3 mm1.4 mm-CeramicAEC - Q200B82498FReel , Cut Tape
L08054R7DEWTR


RF Inductors - SMD 4.7nH
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Kyocera AVX 5757
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 1.0395

Multiples of: 1

Thin Film0805 (2012 METRIC)Unshielded4.7 nH0.5 nH1.5 A100 mOhms-- 55 C+ 125 C435.5 GHzStandard2.11 mm1.5 mm0.91 mm-  0603, 0805Reel , Cut Tape
LQW18AN9N9G80D


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 5755
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.118

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded9.9 nH2 %1.6 A52 mOhms-- 55 C+ 125 C384.75 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
MCQ1V2012-R150-R


RF Inductors - SMD Multi H Q,IND 150nH Q20 250mA 2PADS SMT
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Eaton 5754
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0238

Multiples of: 1

Multilayer0805 (2012 METRIC)Unshielded150 nH10 %250 mA250 mOhms-- 40 C+ 85 C20200 MHzStandard2 mm1.2 mm0.9 mm-  MCQ1VReel , Cut Tape
LQW18ASR18G0CD


RF Inductors - SMD Fixed IND 180nH 240mA NONAUTO
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Murata 5754
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2787

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded180 nH2 %240 mA1.4 Ohms-- 55 C+ 125 C25990 MHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
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