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
  
                         
LQW15AN4N1B8ZD


RF Inductors - SMD
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Murata 9700
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AUD 0.1535
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Wirewound0402 (1005 METRIC)Unshielded4.1 nH0.1 nH1.8 A44 mOhms-- 55 C+ 125 C309.6 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
AISC-0402-4N7G-T


RF Inductors - SMD FIXED IND 4.7NH 800MA 83 MOHM
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ABRACON 9700
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AUD 0.1641
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 0402 (1005 METRIC)Unshielded4.7 nH2 %1 A130 mOhms - 40 C+ 125 C204775 MHz     Ceramic Aisc - 0402Reel
CW105550A-27NJ


RF Inductors - SMD 27nH 5 0.4A AEC-Q200
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Bourns 9700
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AUD 0.1609
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Wirewound Unshielded27 nH5 %400 mA298 mOhms-- 40 C+ 125 C262.48 GHzStandard1 mm0.55 mm0.5 mm-CeramicAEC - Q200CW105550AReel , Cut Tape
CW100505-5N6J


RF Inductors - SMD 56.0 nH 5% 250 MHz 0.083ohms
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Bourns 9700
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AUD 0.1766
Multiples of: 10000

RF Choke0402 (1005 METRIC)Unshielded56 nH5 %760 mA83 mOhms-- 55 C+ 125 C235.8 GHzStandard1 mm0.55 mm0.5 mm-Ceramic CW100505Reel
IWC1008FR10R-3G


RF Inductors - SMD 1008 100nH 2% 650mA
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Laird Performance Materials 9700
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AUD 0.1846
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Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded100 nH2 %650 mA560 mOhms-- 40 C+ 125 C601 GHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
MHQ1005P3N0BTD25


RF Inductors - SMD IND 0402 3.0nH S-HQ AEC Q200 RF IND
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TDK 9700
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AUD 0.21
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Multilayer0402 (1005 METRIC)Unshielded3 nH0.1 nH900 mA80 mOhms-- 55 C+ 125 C239.4 GHzStandard1 mm0.5 mm0.6 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
AIAC-1812-27NK-T


RF Inductors - SMD FIXED IND 27NH 3.5A 4.6 MOHM SMD
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ABRACON 9700
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AUD 0.3427
Multiples of: 2000

SMT Air Coil Inductor1812 (4532 METRIC)Unshielded27 nH10 %3.5 A4.6 mOhms - 40 C+ 125 C1002.7 GHzStandard4.7 mm3.5 mm3.5 mm Air AIAC - 1812Reel , Cut Tape
MHQ1005P43NJTD25


RF Inductors - SMD IND 0402 43nH S-HQ AEC Q200 RF IND
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TDK 9698
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AUD 0.1188
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Multilayer0402 (1005 METRIC)Unshielded43 nH5 %190 mA1.6 Ohms-- 55 C+ 125 C222 GHzStandard1 mm0.5 mm0.6 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
ATFC-0201HQ-0N1B-T


RF Inductors - SMD FIXED IND 0.1NH 850MA 50 MOHM
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ABRACON 9697
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AUD 0.0565
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Thin Film Chip Inductor0201 (0603 METRIC)Unshielded100 pH0.1 nH850 mA50 mOhms - 40 C+ 85 C146 GHzStandard0.6 mm0.3 mm0.23 mm Ceramic ATFC - 0201HQReel , Cut Tape
MHQ1005P22NJTD25


RF Inductors - SMD IND 0402 22nH S-HQ AEC Q200 RF IND
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TDK 9697
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AUD 0.1188
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Multilayer0402 (1005 METRIC)Unshielded22 nH5 %230 mA1.1 Ohms-- 55 C+ 125 C202.9 GHzStandard1 mm0.5 mm0.6 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
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