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-4N7D-T


RF Inductors - SMD IND 4.7nH 1.5A 70m?
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Abracon 3855
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AUD 0.1697
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Wirewound0402 (1208 METRIC)Unshielded4.7 nH0.5 nH1.5 A700 mOhms - 40 C+ 125 C836.85 GHzStandard1.27 mm0.76 mm0.61 mm Ceramic AISC - Q0402HQReel , Cut Tape
WCLA2520V1-3R3-R


RF Inductors - SMD Chip IND 3.3uH 0.715A SMT 2 Pad
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Eaton 3855
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AUD 0.2529
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Wirewound1008 (2520 METRIC)Shielded3.3 uH10 %715 mA260 mOhms - 55 C+ 125 C1248 MHz 2.9 mm2.5 mm2.1 mm Ferrite WCLAReel , Cut Tape
B82432C1473J000


RF Inductors - SMD SMT-INDUCTOR 1812 47UH 5%, AEC-Q200
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TDK 3855
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AUD 0.8177
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Wirewound1812 (4532 METRIC)Unshielded47 uH5 %210 mA2.3 Ohms-- 55 C+ 150 C3012 MHzStandard4.5 mm3.2 mm3.2 mm-FerriteAEC - Q200B82432CReel , Cut Tape
WCLA2520V1-330-R


RF Inductors - SMD Chip IND 33.0uH 0.236A SMT 2 Pad
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Eaton 3854
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AUD 0.2529
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Wirewound1008 (2520 METRIC)Shielded33 uH10 %236 mA2.47 mOhms - 55 C+ 125 C1215 MHz 2.9 mm2.5 mm2.1 mm Ferrite WCLAReel , 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 3850
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AUD 0.0723
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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
LQW18AS4N3J0ZD


RF Inductors - SMD
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Murata 3850
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AUD 0.1202
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Wirewound0603 (1608 METRIC)Unshielded4.3 nH5 %700 mA63 mOhms-- 40 C+ 125 C225.9 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
AWCM0016100862NJ00


RF Inductors - SMD Chilisin RF inductor Wire Wound-STD
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Pulse 3850
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AUD 0.1226
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 1.6 mm x 1.02 mm x 0.82 mmUnshielded62 nH5 %280 mA510 mOhms - 40 C+ 125 C382.3 GHzStandard1.6 mm1.02 mm0.82 mm  AEC - Q200AWCMReel , Cut Tape
AISC-Q0402HQ-3N6C-T


RF Inductors - SMD IND 3.6nH 1.7A 45m?
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Abracon 3850
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AUD 0.176
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Wirewound0402 (1208 METRIC)Unshielded3.6 nH0.2 nH1.7 A45 mOhms - 40 C+ 125 C9411.7 GHzStandard1.27 mm0.76 mm0.61 mm Ceramic AISC - Q0402HQReel , Cut Tape
AISC-Q0402HQ-6N2G-T


RF Inductors - SMD IND 6.2nH 1.6A 55m?
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Abracon 3850
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AUD 0.176
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Wirewound0402 (1208 METRIC)Unshielded6.2 nH2 %1.6 A55 mOhms - 40 C+ 125 C1005.8 GHzStandard1.27 mm0.76 mm0.61 mm Ceramic AISC - Q0402HQReel , Cut Tape
0603AQC-3N9K-01


RF Inductors - SMD Wire-wound Ceramic Chip Inductor AEC-200
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Fastron 3850
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AUD 0.2231
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Chip Inductor0603 (1608 METRIC)Unshielded3.9 nH10 %3.5 A25 mOhms - 40 C+ 140 C5010 GHzStandard1.7 mm1.12 mm1.05 mm CeramicAEC - Q200 Reel , Cut Tape
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