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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Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
AISC-1210HS-4R7K-T2


RF Inductors - SMD FIXED IND 4.7UH 550MA 950 MOHM
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ABRACON 1046
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.1948

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded4.7 uH10 %550 mA950 mOhms600 mA- 40 C+ 85 C1080 MHzStandard3.2 mm3.05 mm1.3 mm Ferrite AISC - 1210HSReel , Cut Tape
AIAC-1008C-6N8K-T


RF Inductors - SMD FIXED IND 6.8NH 1.2A 4 MOHM SMD
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ABRACON 567
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.7827

Multiples of: 1

SMT Air Coil Inductor1008 (2520 METRIC)Unshielded6.8 nH10 %1.2 A4 mOhms - 40 C+ 125 C803 GHzStandard3.2 mm1.9 mm2.2 mm Air AIAC - 1008CReel , Cut Tape
4232-393K


RF Inductors - SMD factory currently not accepting orders
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

API Delevan 567
Ships to you
between Tue. 21 Jul to Thu. 23 Jul
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AUD 2.7755

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Wirewound Unshielded39 uH10 %139 mA10.8 Ohms-- 55 C+ 125 C3012 MHzStandard3.51 mm2.67 mm2.57 mm-Iron 4232/RReel , Cut Tape
MCLA2012V1-3R9-R


RF Inductors - SMD MCLA Auto Chip IND 2012 3.9uH 2 Pads
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Eaton 566
Ships to you
between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.0604

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Multilayer0805 (2012 METRIC)Unshielded3.9 uH10 %50 mA800 mOhms-- 40 C+ 125 C3541 MHzStandard2 mm1.2 mm0.9 mm- AEC - Q200MCLAReel , Cut Tape
1210F-2R7K-01


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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Fastron 565
Ships to you
between Wed. 15 Jul to Tue. 21 Jul
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AUD 0.3379

Multiples of: 1

Wirewound3.8 mm x 3 mm x 2.4 mmUnshielded2.7 uH10 %450 mA490 mOhms - 40 C+ 85 C30150 MHzStandard3.8 mm3 mm2.4 mm FerriteAEC - Q2001210FReel
LQW32FT2R7M0HL


2.7uH ±20% 1210 Inductors (SMD) ROHS
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Murata 561
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.7844

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Wirewound Unshielded2.7 uH20 %975 mA220 mOhms975 mA- 40 C+ 125 C-200 MHzStandard3.2 mm2.5 mm2.3 mm-FerriteAEC - Q200LQW32FT_0HReel , Cut Tape
NLCV32T-6R8M-EFD


RF Inductors - SMD 6.8uH 0.27ohms 530mA 3.2x2.5mm AEC-Q200
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TDK 557
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between Wed. 29 Jul to Mon. 03 Aug
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AUD 0.0937

Multiples of: 5

Wirewound1210 (3225 METRIC)Unshielded6.8 uH20 %530 mA270 mOhms-- 40 C+ 105 C1538 MHzStandard3.2 mm2.5 mm2.4 mm-FerriteAEC - Q200NLCV25 - EFDReel , Cut Tape
PE-0603CLHR47STS


RF Inductors - SMD 0603 470nH 1050mA DCR=130mOhms RF
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Pulse 515
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.1327

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Multilayer0603 (1608 METRIC)Shielded470 nH-1.05 A130 mOhms800 mA- 40 C+ 85 C-100 MHzStandard1.6 mm0.8 mm0.8 mm-Ceramic PE - 0603CLHReel , Cut Tape
AISC-0805-R039J-T


RF Inductors - SMD FIXED IND 39NH 500MA 290 MOHM
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ABRACON 369
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between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.3086

Multiples of: 1

Wirewound0805 (2317 METRIC)Unshielded39 nH5 %500 mA290 mOhms - 40 C+ 125 C602 GHzStandard2.29 mm1.73 mm1.55 mm Ceramic AISC - 0805Reel , Cut Tape
LQH44PN3R3MPRL


RF Inductors - SMD 3.3uH 2300mA 20%
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Murata 31
Ships to you
between Tue. 21 Jul to Thu. 23 Jul
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AUD 0.284

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Wirewound4 mm x 4 mm x 1.65 mmUnshielded3.3 uH20 %2.3 A55 mOhms - 40 C+ 125 C 40 MHzStandard4 mm4 mm1.65 mm   LQH44PN_PRReel , Cut Tape
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