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
  
                         
LQG15HSR27H02D


RF Inductors - SMD
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Murata 1182
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.0404

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Multilayer0402 (1005 METRIC)Unshielded270 nH3 %110 mA4.94 Ohms-- 55 C+ 125 C8400 MHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
IC0805B182R-10


RF Inductors - SMD 1800nH 0.6ohms 50mA
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Laird Connectivity 1172
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AUD 0.1428

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Signal Filter0805 (2012 METRIC)Unshielded1.8 uH10 %50 mA600 mOhms-- 40 C+ 125 C4555 MHzStandard2 mm1.25 mm0.9 mm-Ferrite IC0805Reel , Cut Tape
AISC-1210-8R6J-T


RF Inductors - SMD FIXED IND 8.6UH 200MA 9 OHM SMD
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ABRACON 1172
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AUD 0.4748

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Wirewound1210 (3225 METRIC)Unshielded8.6 uH5 %200 mA9 Ohms - 40 C+ 125 C1540 MHzStandard3.65 mm2.95 mm2.7 mm Ceramic AISC - 1210Reel , Cut Tape
NLCV32T-470K-EFD


RF Inductors - SMD 47uH 1.64ohms 180mA 3.2x2.5mm AEC-Q200
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TDK 1164
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AUD 0.1055

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Wirewound1210 (3225 METRIC)Unshielded47 uH10 %180 mA1.64 Ohms-- 40 C+ 105 C1514 MHzStandard3.2 mm2.5 mm2.4 mm-FerriteAEC - Q200NLCV25 - EFDReel , Cut Tape
IMC1008ER22NJ


RF Inductors - SMD 22nH 5%
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Vishay 1157
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AUD 0.1855

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Wirewound1008 (2520 METRIC)Unshielded22 nH5 %1 A100 mOhms-- 40 C+ 125 C602.5 GHzStandard2.5 mm2 mm1.6 mm-Ceramic IMCReel , Cut Tape
NLV25T-4R7J-EF


RF Inductors - SMD 4.7uH 2.3ohms 175mA Wound Ferrite
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TDK 1144
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AUD 0.0227

Multiples of: 10

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded4.7 uH5 %175 mA2.3 Ohms-- 40 C+ 105 C3043 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
NLV32T-391J-EF


RF Inductors - SMD 390uH 36ohms 35mA Wound Ferrite
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TDK 1144
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AUD 0.0513

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Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded390 uH5 %35 mA36 Ohms-- 40 C+ 105 C205 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
NLV25T-330J-EF


RF Inductors - SMD 33uH 7.1ohms 110mA Wound Ferrite
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TDK 1076
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AUD 0.0223

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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded33 uH5 %110 mA7.1 Ohms-- 40 C+ 105 C2520 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
NLCV32T-1R0M-EF


RF Inductors - SMD INDUCTOR-COIL FXD 1UH +-20%
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TDK 989
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between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.0567

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Wirewound1210 (3225 METRIC)Unshielded1 uH20 %1 A60 mOhms-- 40 C+ 105 C10100 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFReel , Cut Tape
LQG15HS1N1B02D


RF Inductors - SMD 1.1 NH +/-0.1NH
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Murata 921
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between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.0343

Multiples of: 10

Multilayer0402 (1005 METRIC)Unshielded1.1 nH0.1 nH1 A70 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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