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
  
                         
IMC1008ER3N3S


RF Inductors - SMD 3.3nH 9.1%
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Vishay 1101
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.2039

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded3.3 nH0.3 nH1 A60 mOhms-- 40 C+ 125 C506 GHzStandard2.5 mm2 mm1.6 mm-Ceramic IMCReel , Cut Tape
IMC1812ER100K


RF Inductors - SMD 10uH 10%
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Vishay 1099
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.8232

Multiples of: 1

Wirewound1812 (4532 METRIC)Unshielded10 uH10 %250 mA1.6 Ohms-- 55 C+ 125 C5020 MHzStandard4.5 mm3.2 mm3.2 mm-  IMCReel , Cut Tape
NLFV32T-220K-EFT


RF Inductors - SMD 22uH 0.4ohms 120mA +/-10%
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TDK 1098
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.2868

Multiples of: 1

Wirewound1210 (3225 METRIC)Shielded22 uH10 %120 mA400 mOhms-- 40 C+ 105 C--Standard3.2 mm2.5 mm2.2 mm-Ferrite NLFV - EFTReel , Cut Tape
NLCV25T-4R7M-EF


RF Inductors - SMD 4.7uH 1.04ohms 285mA Wound Ferrite
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TDK 1096
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between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.0221

Multiples of: 10

Wirewound1008 (2520 METRIC)Unshielded4.7 uH20 %285 mA800 mOhms-- 40 C+ 105 C20-Standard2.5 mm2 mm1.9 mm Ferrite NLCV - EFReel , Cut Tape
1210R-563J


RF Inductors - SMD 56uH 5%
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API Delevan 1096
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 2.5372

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded56 uH5 %152 mA8 Ohms-- 55 C+ 125 C3011 MHzStandard3.51 mm2.67 mm2.57 mm-Ferrite 1210/RReel , Cut Tape
MCQ1V2012-R100-R


RF Inductors - SMD Multi H Q,IND 100nH Q20 250mA 2PADS SMT
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Eaton 1094
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.0238

Multiples of: 1

Multilayer0805 (2012 METRIC)Unshielded100 nH10 %250 mA200 mOhms-- 40 C+ 85 C20235 MHzStandard2 mm1.2 mm0.9 mm-  MCQ1VReel , Cut Tape
NLCV32T-151K-EFD


RF Inductors - SMD 150uH 6.1ohms 100mA 3.2x2.5mm AEC-Q200
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TDK 1091
Ships to you
between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.1251

Multiples of: 5

Wirewound1210 (3225 METRIC)Unshielded150 uH10 %100 mA6.1 Ohms-- 40 C+ 105 C208 MHzStandard3.2 mm2.5 mm2.4 mm-FerriteAEC - Q200NLCV25 - EFDReel , Cut Tape
PM105SB-330L-RC


Inductor Power Shielded Bobbin Core 33uH 15% 100KHz 27Q-Factor Ferrite 1.2A 110mOhm DCR T/R
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Bourns 1087
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.7719

Multiples of: 1

Wirewound Shielded33 uH15 %1.2 A110 mOhms-- 30 C+ 100 C2714 MHzStandard4.5 mm--9.9 mmFerrite PM105SBReel , Cut Tape
LQW18AN8N7D00D


RF Inductors - SMD 8.7 NH
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Murata 339
Ships to you
between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.0457

Multiples of: 10

Wirewound0603 (1608 METRIC)Unshielded8.7 nH0.5 nH650 mA110 mOhms-- 55 C+ 125 C356 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
NLV32T-100J-EFD


RF Inductors - SMD 10uH 2.1ohms 150mA Wound Fer AEC-Q200
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TDK 111
Ships to you
between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.1226

Multiples of: 5

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded10 uH5 %150 mA2.1 Ohms-- 40 C+ 105 C3030 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
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