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
  
                         
LQW18AN3N6D00D


RF Inductors - SMD 3.6 NH +-.5NH
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Murata 5908
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between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.0793

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded3.6 nH0.5 nH850 mA59 mOhms-- 55 C+ 125 C256 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
B82422H1102K


RF Inductors - SMD 1uH 1150mA 10% 3.2x2.5mm SMD
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TDK 4074
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between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.3706

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Wirewound1210 (3225 METRIC)Unshielded1 uH10 %1.15 A100 mOhms1.835 A- 55 C+ 150 C8150 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200B82422HReel , Cut Tape
AISC-0603-R051G-T


RF Inductors - SMD FIXED IND 51NH 390MA 300 MOHM
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ABRACON 2293
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between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.1706

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Wirewound0603 (1812 METRIC)Unshielded51 nH2 %390 mA300 mOhms - 40 C+ 125 C352.4 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - 0603Reel , Cut Tape
IMC1210ERR39K


RF Inductors - SMD 39uh 10%
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Vishay 1881
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between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.921

Multiples of: 1

Molded1210 (3225 METRIC) 390 nH10 %450 mA450 mOhms - 55 C+ 125 C30250 MHzStandard      IMCReel , Cut Tape
NLV32T-680J-EFD


RF Inductors - SMD 68uH 9.0ohms 50mA Wound Fer AEC-Q200
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TDK 1876
Ships to you
between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.1638

Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded68 uH5 %50 mA9 Ohms-- 40 C+ 105 C3012 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
LQW2UAS82NF00L


RF Inductors - SMD 82 NH 1%
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Murata 1874
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between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.3247

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded82 nH1 %1 A220 mOhms-- 55 C+ 125 C601 GHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
LQG15HS1N5B02D


RF Inductors - SMD 1.5 NH +/-0.1NH
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Murata 1873
Ships to you
between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.0414

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded1.5 nH0.1 nH1 A70 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
IMC1008ER2R7J


RF Inductors - SMD 2.7uH 5%
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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.

Vishay 1866
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between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.208

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded2.7 uH5 %195 mA2.6 Ohms-- 40 C+ 125 C20130 MHzStandard2.5 mm2 mm1.6 mm-Ferrite IMCReel , Cut Tape
LQW15CAR11J00D


RF Inductors - SMD
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Murata 1829
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between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.3293

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded110 nH5 %900 mA130 mOhms-- 40 C+ 125 C-1.6 GHzStandard1 mm0.5 mm0.5 mm-Ferrite LQWReel , Cut Tape
LQW15AN2N7C8ZD


RF Inductors - SMD
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Murata 464
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between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.1155

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded2.7 nH0.2 nH1.5 A47 mOhms-- 55 C+ 125 C2814 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
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