About RF inductors - SMD

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
  
                         
LQG15HH2N2B02D


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 Availability : 9700
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USD 0.0728

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Multilayer0402 (1005 METRIC)Unshielded2.2 nH0.1 nH900 mA90 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQW18AN12NG1ZD


RF Inductors - SMD
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Murata Availability : 7642
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USD 0.0797

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded12 nH2 %750 mA71 mOhms-- 55 C+ 125 C385 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
CW105550A-24NJ


RF Inductors - SMD 24nH 5 0.4A AEC-Q200
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Bourns Availability : 0
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USD 0.0781

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Wirewound Unshielded24 nH5 %400 mA300 mOhms-- 40 C+ 125 C252.7 GHzStandard1 mm0.55 mm0.5 mm-CeramicAEC - Q200CW105550AReel
LQW15AN2N3B8ZD


RF Inductors - SMD
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Murata Availability : 0
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USD 0.0782

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Wirewound0402 (1005 METRIC)Unshielded2.3 nH0.1 nH2.53 A22 mOhms-- 55 C+ 125 C3015.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
IWC0603F68NR-3G


RF Inductors - SMD 0603 68nH 2% 600mA
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Laird Performance Materials Availability : 0
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USD 0.0784

Multiples of: 20000

Wirewound1.8 mm x 1.12 mm x 1.02 mmUnshielded68 nH2 %600 mA340 mOhms-- 40 C+ 125 C371.7 GHzStandard1.8 mm1.12 mm1.02 mm-Ceramic IWC0603Reel , Cut Tape
IWC0603AR33R-3G


RF Inductors - SMD 0603 330nH 2% 100mA
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Laird Performance Materials Availability : 0
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USD 0.0784

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Wirewound1.8 mm x 1.12 mm x 1.02 mmUnshielded330 nH2 %100 mA3.9 Ohms-- 40 C+ 125 C25900 MHzStandard1.8 mm1.12 mm1.02 mm-Ceramic IWC0603Reel , Cut Tape
LQP03HQR20H02D


RF Inductors - SMD
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Murata Availability : 0
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USD 0.0786

Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded200 nH3 %75 mA9 Ohms-- 55 C+ 125 C9700 MHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel
0805AS-R18J-08


RF Inductors - SMD Wire-wound Ceramic RF Chip Inductor
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Fastron Availability : 0
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USD 0.0791

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Wirewound0805 (2012 METRIC)Unshielded180 nH5 %400 mA640 mOhms - 40 C+ 150 C50870 MHzStandard2.3 mm1.8 mm1.6 mm CeramicAEC - Q2000805ASReel
LQW15AN6N4G80D


RF Inductors - SMD
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Murata Availability : 0
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USD 0.0794

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Wirewound0402 (1005 METRIC)Unshielded6.4 nH2 %1.38 A65 mOhms - 55 C+ 125 C337 GHzStandard1 mm0.6 mm0.5 mm   LQWReel , Cut Tape
CW105550A-68NJ


RF Inductors - SMD 68nH 5 0.18A AEC-Q200
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Bourns Availability : 0
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USD 0.0794

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Wirewound Unshielded68 nH5 %180 mA1.12 Ohms-- 40 C+ 125 C221.62 GHzStandard1 mm0.55 mm0.5 mm-CeramicAEC - Q200CW105550AReel , Cut Tape
LQW04AN1N7D00D


RF Inductors - SMD
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Murata Availability : 0
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USD 0.0795

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   1.7 nH0,5nH                
MHL1JCTTDR12J


RF Inductors - SMD 120nH 5%
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KOA Speer Availability : 0
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USD 0.0796

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Multilayer0603 (1608 METRIC)Unshielded120 nH5 %300 mA1.3 Ohms - 55 C+ 125 C 700 MHzStandard1.6 mm0.8 mm0.8 mm   MHLReel , Cut Tape
LQW15AN8N0J8ZD


RF Inductors - SMD
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Murata Availability : 0
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USD 0.0803

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Wirewound0402 (1005 METRIC)Unshielded8 nH5 %1.7 A50 mOhms - 55 C+ 125 C307 GHzStandard1 mm0.6 mm0.5 mm  AEC - Q200LQWReel , Cut Tape
BWCM0016100882NG00


RF Inductors - SMD Chilisin RF inductor Wire Wound-STD
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Pulse Availability : 0
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USD 0.0803

Multiples of: 4000

 1.6 mm x 1.02 mm x 0.82 mmUnshielded82 nH2 % 600 mOhms250 mA- 55 C+ 125 C342 GHzStandard1.6 mm1.02 mm0.82 mm Ceramic BWCMReel , Cut Tape
MLF1608DR68KTD25


RF Inductors - SMD 680nH 1.25ohms 70mA +/-10% Fer AEC-Q200
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TDK Availability : 0
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USD 0.0809

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Multilayer0603 (1608 METRIC)Shielded680 nH10 %70 mA1.25 Ohms-- 55 C+ 125 C15210 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
MLF1608E120MTD25


RF Inductors - SMD 12uH 1.8ohms 10mA +/-20% Fer AEC-Q200
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TDK Availability : 0
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USD 0.0811

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Multilayer0603 (1608 METRIC)Shielded12 uH20 %10 mA1.8 Ohms-- 55 C+ 125 C3045 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
MLF1005VR15KT000


RF Inductors - SMD 1mm x 0.5mm x 0.5mm, -55 to +125 degC, 180mA, 0.15?H, 630mohm
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TDK Availability : 0
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USD 0.0811

Multiples of: 1

Multilayer0402 (1005 METRIC)Shielded150 nH10 %180 mA630 mOhms-- 55 C+ 125 C15650 MHzStandard1 mm0.5 mm0.5 mm-Ferrite MLFReel , Cut Tape
IWC0805E68NR-3G


RF Inductors - SMD 0805 68nH 2% 500mA
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Laird Performance Materials Availability : 0
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USD 0.0818

Multiples of: 10000

Wirewound2.35 mm x 1.73 mm x 1.52 mmUnshielded68 nH2 %500 mA380 mOhms-- 40 C+ 125 C601.35 GHzStandard2.35 mm1.73 mm1.52 mm-Ceramic IWC0805Reel , Cut Tape
IWC0805D82NR-3G


RF Inductors - SMD 0805 82nH 2% 400mA
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Laird Performance Materials Availability : 0
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USD 0.0818

Multiples of: 10000

Wirewound2.35 mm x 1.73 mm x 1.52 mmUnshielded82 nH2 %400 mA420 mOhms-- 40 C+ 125 C651.3 GHzStandard2.35 mm1.73 mm1.52 mm-Ceramic IWC0805Reel , Cut Tape
IWC0805DR15R-3G


RF Inductors - SMD 0805 150nH 2% 400mA
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Laird Performance Materials Availability : 0
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USD 0.0818

Multiples of: 10000

Wirewound2.35 mm x 1.73 mm x 1.52 mmUnshielded150 nH2 %400 mA560 mOhms-- 40 C+ 125 C50900 MHzStandard2.35 mm1.73 mm1.52 mm-Ceramic IWC0805Reel , Cut Tape
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