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
  
                         
AIAC-1812-68NJ-T


RF Inductors - SMD FIXED IND 68NH 2.9A 8.1 MOHM SMD
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ABRACON 2046
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AUD 0.7279
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SMT Air Coil Inductor1812 (4532 METRIC)Unshielded68 nH5 %2.9 A8.1 mOhms - 40 C+ 125 C1001.5 GHzStandard4.7 mm3.5 mm3.5 mm Air AIAC - 1812Reel , Cut Tape
AISC-1210-1R0J-T


RF Inductors - SMD FIXED IND 1UH 320MA 1.85 OHM SMD
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ABRACON 2041
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AUD 0.528
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Wirewound1210 (3225 METRIC)Unshielded1 uH5 %320 mA1.85 Ohms - 40 C+ 125 C45340 MHzStandard3.65 mm2.95 mm2.7 mm Ceramic AISC - 1210Reel , Cut Tape
AIAC-1008C-6N8K-T


RF Inductors - SMD FIXED IND 6.8NH 1.2A 4 MOHM SMD
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ABRACON 2041
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AUD 0.715
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SMT Air Coil Inductor1008 (2520 METRIC)Unshielded6.8 nH10 %1.2 A4 mOhms - 40 C+ 125 C803 GHzStandard3.2 mm1.9 mm2.2 mm Air AIAC - 1008CReel , Cut Tape
LQW18AS8N2G00D


RF Inductors - SMD
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Murata 2039
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AUD 0.0862
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Wirewound0603 (1608 METRIC)Unshielded8.2 nH2 %700 mA115 mOhms-- 40 C+ 125 C304.2 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQP03TN5N6J02D


RF Inductors - SMD
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Murata 2037
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AUD 0.0081
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded5.6 nH5 %350 mA400 mOhms-- 55 C+ 125 C144 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQW2UAS8R2J0CL


RF Inductors - SMD
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Murata 2035
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AUD 0.18
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Multilayer Unshielded8.2 uH5 %170 mA6 Ohms-- 40 C+ 85 C1825 MHzStandard2.62 mm2.45 mm1.83 mm-Metal LQWReel , Cut Tape
CW252016-R47J


Inductor RF Wirewound 0.47uH 5% 25.2MHz 45Q-Factor Ceramic 0.47A 1.19Ohm DCR 1008 T/R
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Bourns 2030
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AUD 0.1794
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Wirewound1008 (2520 METRIC)Unshielded470 nH5 %470 mA1.19 Ohms-- 40 C+ 125 C45450 MHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
1206F-8R2K-01


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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Fastron 2025
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AUD 0.3657
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Wirewound1206 (3216 METRIC)Unshielded8.2 uH10 %220 mA3.1 Ohms     Standard    FerriteAEC - Q2001206FReel , Cut Tape
MLF2012A3R3JT000


RF Inductors - SMD 2mm x 1.25mm x 1.25mm, -55 to +125 degC, 50mA, 3.3?H, 600mohm
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TDK 2017
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AUD 0.047
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Multilayer0805 (2012 METRIC)Shielded3.3 uH5 %50 mA600 mOhms-- 55 C+ 125 C4590 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
LQW15AN5N8B00D


RF Inductors - SMD 5.8 NH +-.1NH
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Murata 1988
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AUD 0.0443
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Wirewound0402 (1005 METRIC)Unshielded5.8 nH0.1 nH700 mA120 mOhms-- 55 C+ 125 C258 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
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