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-Q0402HQ-22NG-T


RF Inductors - SMD IND 22nH 0.8A 160m?
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Abracon 3876
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AUD 0.1981
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Wirewound0402 (1208 METRIC)Unshielded22 nH2 %800 mA160 mOhms - 40 C+ 125 C743.3 GHzStandard1.27 mm0.76 mm0.61 mm Ceramic AISC - Q0402HQReel , Cut Tape
WCL3225-101-R


RF Inductors - SMD WCL Chip IND 3225 100uH 2 Pads
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Eaton 3876
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AUD 0.2221
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Wirewound1210 (3225 METRIC)Unshielded100 uH5 %95 mA6.8 Ohms-- 40 C+ 85 C85 MHzStandard3.5 mm2.9 mm2.25 mm-  WCLReel , Cut Tape
LQG18HH39NJ00D


RF Inductors - SMD
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Murata 3875
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AUD 0.101
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Multilayer0603 (1608 METRIC)Unshielded39 nH5 %400 mA600 mOhms-- 55 C+ 125 C121 GHzStandard1.6 mm0.8 mm0.8 mm-AirAEC - Q200LQGReel , Cut Tape
AISC-Q0402-20NG-T


RF Inductors - SMD IND 20nH 0.42A 250m?
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Abracon 3875
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AUD 0.1638
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded20 nH2 %420 mA250 mOhms - 40 C+ 125 C253 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
B82422H1103J000


RF Inductors - SMD SMT-INDUCTOR 1210-H 10 UH 5%, AEC-Q200
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TDK 3875
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AUD 0.392
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Wirewound1210 (3225 METRIC)Unshielded10 uH5 %500 mA480 mOhms620 mA- 55 C+ 150 C1230 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200B82422HReel , Cut Tape
LQW18AN91NJ8ZD


RF Inductors - SMD
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Murata 3874
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AUD 0.1616
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Wirewound0603 (1608 METRIC)Unshielded91 nH5 %520 mA540 mOhms-- 55 C+ 125 C331.9 GHzStandard1.65 mm0.99 mm0.9 mm- AEC - Q200LQWReel , Cut Tape
HLC021R0BTTR


RF Inductors - SMD 1.0nH
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Kyocera AVX 3874
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AUD 0.2273
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Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded1 nH0.1 nH800 mA100 mOhms-- 55 C+ 125 C2520 GHzStandard1 mm0.58 mm0.35 mm-  HLCReel , Cut Tape
LQW15AN5N0C00D


RF Inductors - SMD
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Murata 3871
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AUD 0.0989
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Wirewound0402 (1005 METRIC)Unshielded5 nH0.2 nH600 mA120 mOhms-- 55 C+ 125 C258 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQW18ANR13G0ZD


RF Inductors - SMD
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Murata 3871
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AUD 0.1222
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Wirewound0603 (1608 METRIC)Unshielded130 nH2 %170 mA1.4 Ohms-- 55 C+ 125 C321.45 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
MLF1608A1R5MTA00


RF Inductors - SMD 1.6mm x 0.8mm x 0.8mm, -55 to +125 degC, 50mA, 1.5?H, 700mohm
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TDK 3870
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AUD 0.08
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Multilayer  1.5 uH20 %50 mA700 mOhms - 55 C+ 125 C 140 KHzStandard1.6 mm0.8 mm0.95 mm   MLFReel , Cut Tape
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