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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(Ex. GST)(▲▼)		Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
AISC-0402-15NJ-T


15 nH Unshielded Drum Core, Wirewound Inductor 560 mA 170mOhm Max 0402 (1005 Metric)
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ABRACON 13181
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AUD 0.1706
Multiples of: 1

Ceramic Wirewound RF Inductor0402 (1005 METRIC)Unshielded15 nH5 %560 mA170 mOhms   263.28 GHzStandard1.1 mm0.6 mm0.66 mm Ceramic AISC - 0402Reel , Cut Tape
IMC1008ER12NJ


RF Inductors - SMD 12nH 5%
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Vishay 1622
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AUD 0.1958
Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded12 nH5 %1 A80 mOhms-- 40 C+ 125 C603.6 GHzStandard2.5 mm2 mm1.6 mm-Ceramic IMCReel , Cut Tape
NLV25T-4R7J-EFD


RF Inductors - SMD 4.7uH 2.3ohms 175mA Wound Fer AEC-Q200
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TDK 1621
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AUD 0.1517
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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-FerriteAEC - Q200NLV25 - EFDReel , Cut Tape
LQW18ANR15J80D


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 1616
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AUD 0.0965
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Wirewound0603 (1608 METRIC)Unshielded150 nH5 %420 mA870 mOhms - 55 C+ 125 C281.58 GHzStandard1.65 mm0.99 mm0.9 mm   LQWReel , Cut Tape
AISC-0805-R039G-T


RF Inductors - SMD FIXED IND 39NH 500MA 290 MOHM
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Abracon 1615
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AUD 0.35
Multiples of: 1

Wirewound0805 (2317 METRIC)Unshielded39 nH2 %500 mA290 mOhms - 40 C+ 125 C602 GHzStandard2.29 mm1.73 mm1.55 mm Ceramic AISC - 0805Reel , Cut Tape
MCLA1608V1-1R5-R


RF Inductors - SMD 1.5 UH 10% AEC-Q200
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Eaton 1611
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AUD 0.0569
Multiples of: 1

Multilayer0603 (1608 METRIC)Unshielded1.5 uH10 %25 mA700 mOhms-- 40 C+ 125 C2565 MHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200MCLAReel , Cut Tape
CW160808-10NJ


Inductor RF Wirewound 0.01uH 5% 250MHz 30Q-Factor Alumina 0.7A 0.13Ohm DCR 0603 T/R
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Bourns 1609
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AUD 0.1974
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded10 nH5 %700 mA130 mOhms-- 40 C+ 125 C304.8 GHzStandard1.65 mm1.05 mm1 mm-Ceramic CW160808Reel , Cut Tape
MLF2012A3R9JTD25


RF Inductors - SMD 3.9uH 650mohms 30mA +/-5% Fer AEC-Q200
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TDK 1590
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AUD 0.1479
Multiples of: 5

Multilayer inductor  3.9 uH5 %                
NLCV32T-4R7M-EFD


RF Inductors - SMD 4.7uH 0.2ohms 620mA 3.2x2.5mm AEC-Q200
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TDK 1324
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AUD 0.0971
Multiples of: 5

Wirewound1210 (3225 METRIC)Unshielded4.7 uH20 %620 mA200 mOhms-- 40 C+ 105 C1546 MHzStandard3.2 mm2.5 mm2.4 mm-FerriteAEC - Q200NLCV25 - EFDReel , Cut Tape
NLV32T-1R5J-EF


RF Inductors - SMD 1.5uH 850mohms 370mA Wound Ferrite
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TDK 1251
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AUD 0.063
Multiples of: 10

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded1.5 uH5 %370 mA850 mOhms-- 40 C+ 105 C3085 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
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