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
  
                         
LQP03TQ1N8B02D


RF Inductors - SMD 1.8nH 650mA 0201 (0603 metric) SUGGESTED ALT LQP03HQ1N8B02D
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Murata 1774
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AUD 0.0276
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Thin Film0201 (0603 METRIC)Unshielded1.8 nH0.1 nH650 mA100 mOhms-- 55 C+ 125 C1715 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
AISC-0402-47NJ-T


RF Inductors - SMD FIXED IND 47NH 150MA 750 MOHM
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ABRACON 1771
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AUD 0.1638
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Wirewound0402 (1005 METRIC) 47 nH5 %150 mA750 mOhms - 25 C+ 85 C202.1 GHz-1.19 mm0.64 mm0.66 mm Ceramic Aisc - 0402Cut Tape
AIML-0805-5R6K-T


RF Inductors - SMD FIXED IND 5.6UH 15MA 900 MOHM
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ABRACON 1770
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AUD 0.0758
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Multilayer Ferrite Chip Inductor0805 (2012 METRIC)Shielded5.6 uH10 %15 mA900 mOhms - 55 C+ 125 C5032 MHzStandard2 mm1.25 mm0.85 mm Ferrite AIML - 0805Reel , Cut Tape
MLF1608DR68MTD25


RF Inductors - SMD 680nH 1.25ohms 70mA +/-20% Fer AEC-Q200
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TDK 1770
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AUD 0.1155
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Multilayer0603 (1608 METRIC)Shielded680 nH20 %70 mA1.25 Ohms-- 55 C+ 125 C15210 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
BWLD003025226R8J00


RF Inductors - SMD 6.8uH Unshielded 700mA 315mOhms 1210
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Pulse 1766
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AUD 0.1658
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 2.99 mm x 2.5 mm x 2.2 mmUnshielded6.8 uH5 %700 mA315 mOhms - 40 C+ 105 C2028 MHzStandard2.99 mm2.5 mm2.2 mm Ferrite BWLDReel , Cut Tape
AISC-1206-1R2J-T


RF Inductors - SMD FIXED IND 1.2UH 300MA 3.2 OHM
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ABRACON 1766
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AUD 0.2568
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Ceramic Wirewound RF Inductor1206 (3216 METRIC)Unshielded1.2 uH5 %300 mA3.2 Ohms - 40 C+ 125 C45380 MHzStandard3.56 mm2.16 mm1.52 mm Ceramic AISC - 1206Reel , Cut Tape
MHQ0603P20NHTD25


RF Inductors - SMD 0201 20nH Tol 3% AEC-Q200
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TDK 1765
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AUD 0.0741
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Multilayer0201 (0603 METRIC)Unshielded20 nH3 %160 mA2 Ohms-- 55 C+ 125 C163.5 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
LQW15AN8N6J8ZD


RF Inductors - SMD
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Murata 1762
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AUD 0.1352
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Wirewound0402 (1005 METRIC)Unshielded8.6 nH5 %1.42 A70 mOhms-- 55 C+ 125 C316.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
WCL2520-470-R


RF Inductors - SMD WCL Chip IND 2520 47uH 2 Pads
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Eaton 1760
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AUD 0.1543
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Wirewound1008 (2520 METRIC)Unshielded47 uH5 %60 mA5.7 Ohms - 40 C+ 85 C   2.92 mm2.79 mm2.1 mm   WCLReel , Cut Tape
NLFV32T-2R2M-EF


RF Inductors - SMD 3.2mm x 2.5mm x 2.2mm, -40 to +105 degC, 500mA, 2.2?H, 108mohm
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TDK 1644
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AUD 0.1094
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Wirewound1210 (3225 METRIC)Shielded2.2 uH20 %500 mA90 mOhms-- 40 C+ 105 C--Standard3.2 mm2.5 mm2.2 mm-Ferrite NLFV32 - EFReel , Cut Tape
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