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
  
                         
MLF1608A1R8KTD25


RF Inductors - SMD 1.8uH 850mohms 50mA +/-10% Fer AEC-Q200
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TDK 3571
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1344

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Multilayer0603 (1608 METRIC)Shielded1.8 uH10 %50 mA850 mOhms-- 55 C+ 125 C35130 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQG15WZ43NG02D


RF Inductors - SMD Fixed IND 43nH 190mA INFOTMT
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Murata 3568
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1319

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded43 nH2 %190 mA1.6 Ohms-- 55 C+ 125 C221.4 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
MLF2012D68NMT000


RF Inductors - SMD 2mm x 1.25mm x 0.85mm, -55 to +125 degC, 300mA, 0.068?H, 150mohm
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TDK 3560
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0872

Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded68 nH20 %300 mA150 mOhms-- 55 C+ 125 C15600 MHzStandard2 mm1.25 mm0.85 mm-Ferrite MLFReel , Cut Tape
LQW03AW14NJ00D


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 3559
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.4847

Multiples of: 1

Wirewound0201 (0603 METRIC)Unshielded14 nH5 %240 mA530 mOhms-- 55 C+ 125 C376 GHzStandard0.53 mm0.4 mm0.4 mm-  LQWReel , Cut Tape
LQW18AN27NG1ZD


RF Inductors - SMD
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Murata 3556
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1361

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded27 nH2 %590 mA116 mOhms-- 55 C+ 125 C422.8 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
AISC-Q0402-33NG-T


RF Inductors - SMD IND 33nH 0.4A 350m?
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Abracon 3555
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1554

Multiples of: 1

Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded33 nH2 %400 mA350 mOhms - 40 C+ 125 C242.35 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
MHQ0603P15NHTD25


RF Inductors - SMD 0201 15nH Tol 3% AEC-Q200
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TDK 3548
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0748

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded15 nH3 %180 mA1.5 Ohms-- 55 C+ 125 C164.2 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
MHQ0603P2N8BTD25


RF Inductors - SMD 0201 2.8nH Tol 0.1nH AEC-Q200
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TDK 3545
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0814

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded2.8 nH0.1 nH500 mA250 mOhms-- 55 C+ 125 C1610.6 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
LQG18HN2N7S00D


RF Inductors - SMD 2.7 NH +-.3NH
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Murata 3395
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0655

Multiples of: 10

Multilayer0603 (1608 METRIC)Unshielded2.7 nH0.3 nH1 A120 mOhms - 40 C+ 85 C126 GHzStandard1.6 mm0.8 mm0.8 mm-Air LQGReel , Cut Tape
LQW18AN39NG80D


RF Inductors - SMD 39 NH 2%
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Murata 2943
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0954

Multiples of: 5

Wirewound0603 (1608 METRIC)Unshielded39 nH2 %1 A160 mOhms-- 55 C+ 125 C403.28 GHzStandard1.65 mm0.99 mm0.9 mm-- LQWReel , Cut Tape
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