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
  
                         
LQW15AN3N9D1ZD


RF Inductors - SMD
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Murata 9554
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AUD 0.1293
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Wirewound0402 (1005 METRIC)Unshielded3.9 nH0.5 nH750 mA70 mOhms-- 55 C+ 125 C2510 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
AIMC-0402HQ-3N6C-T


RF Inductors - SMD FIXED IND 3.6NH 0.7A 100 MOHM
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Abracon 9552
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AUD 0.1571
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Multilayer Ceramic Chip Inductor0402 (1006 METRIC)Shielded3.6 nH0.2 nH700 mA100 mOhms - 55 C+ 125 C206 GHzStandard1 mm0.6 mm0.5 mm Ceramic AIMC - 0402HQReel , Cut Tape
MLG1005S4N3S


RF Inductors - SMD 4.3nH
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TDK 9550
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AUD 0.0671
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Multilayer0402 (1005 METRIC)Unshielded4.3 nH0.3 nH700 mA200 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , Cut Tape
LQW18AN10NJ0ZD


RF Inductors - SMD
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Murata 9550
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AUD 0.1035
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Wirewound0603 (1608 METRIC)Unshielded10 nH5 %650 mA110 mOhms-- 55 C+ 125 C356 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQW15AN3N8B8ZD


RF Inductors - SMD
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Murata 9548
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AUD 0.1138
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Wirewound0402 (1005 METRIC)Unshielded3.8 nH0.1 nH1.95 A30 mOhms-- 55 C+ 125 C3510 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
MHQ1005P24NGTD25


RF Inductors - SMD IND 0402 24nH S-HQ AEC Q200 RF IND
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TDK 9544
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AUD 0.2019
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Multilayer0402 (1005 METRIC)Unshielded24 nH2 %230 mA1.2 Ohms-- 55 C+ 125 C202.8 GHzStandard1 mm0.5 mm0.6 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
MHQ1005P27NGTD25


RF Inductors - SMD IND 0402 27nH S-HQ AEC Q200 RF IND
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TDK 9544
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AUD 0.2039
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Multilayer0402 (1005 METRIC)Unshielded27 nH2 %230 mA1.3 Ohms-- 55 C+ 125 C202.6 GHzStandard1 mm0.5 mm0.6 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
AIMC-Q0402-10NG-T


RF Inductors - SMD IND 10nH 0.5A 300m?
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Abracon 9543
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AUD 0.0503
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Multilayer Ceramic Chip Inductor0402 (1005 METRIC)Shielded10 nH2 %500 mA300 mOhms - 55 C+ 125 C83.4 GHzStandard1 mm0.5 mm0.5 mm Ceramic AIMC - Q0402Reel , Cut Tape
LQW15AN5N9G8ZD


RF Inductors - SMD
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Murata 9539
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AUD 0.1535
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Wirewound0402 (1005 METRIC)Unshielded5.9 nH2 %1.77 A40 mOhms-- 55 C+ 125 C88 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
BWCS0016100818NG00


RF Inductors - SMD 18nH RDC=0.17OhmS 700mA
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Pulse 9535
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AUD 0.0911
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 1.6 mm x 1.02 mm x 0.82 mmUnshielded18 nH2 %700 mA170 mOhms700 mA- 40 C+ 125 C353.1 GHzStandard1.6 mm1.02 mm0.82 mm Ceramic BWCSReel , Cut Tape
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