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
  
                         
IC0805B182R-10


RF Inductors - SMD 1800nH 0.6ohms 50mA
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Laird Connectivity 16490
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between Wed. 08 Jul to Fri. 10 Jul
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AUD 0.1461

Multiples of: 1

Signal Filter0805 (2012 METRIC)Unshielded1.8 uH10 %50 mA600 mOhms-- 40 C+ 125 C4555 MHzStandard2 mm1.25 mm0.9 mm-Ferrite IC0805Reel , Cut Tape
LQW15CE1R5M10D


RF Inductors - SMD 1.5 UH 20%
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Murata 16488
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between Wed. 08 Jul to Fri. 10 Jul
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AUD 0.1494

Multiples of: 1

 0402 (1006 METRIC)Shielded1.5 uH20 %350 mA1.5 Ohms - 55 C+ 125 C 120 MHz 1 mm0.6 mm0.5 mm   LQW15CE_10Reel , Cut Tape
AIML-0402-1R0K-T


RF Inductors - SMD 1000nH 15mA 5% Tolerance ferrite shielded 0.9 20a.10MHz 40MHz 0402
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ABRACON 16487
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between Wed. 08 Jul to Fri. 10 Jul
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AUD 0.0442

Multiples of: 1

Multilayer Ferrite Chip Inductor0402 (1005 METRIC)Shielded1 uH10 %15 mA900 mOhms - 55 C+ 125 C2040 MHzStandard1 mm0.5 mm0.5 mm Ferrite AIML - 0402Reel , Cut Tape
PE-0402CL1N0STT


RF Inductors - SMD 0402 1nH 400mA DCR=100mOhms RF
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Pulse 16485
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between Wed. 08 Jul to Fri. 10 Jul
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AUD 0.0315

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded1 nH0.3 nH400 mA100 mOhms-- 55 C+ 125 C810 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
MHQ1005P7N5JT000


RF Inductors - SMD IND 0402 7.5nH S-HQ SMD RF IND
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TDK 16485
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between Wed. 08 Jul to Fri. 10 Jul
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AUD 0.0951

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded7.5 nH5 %600 mA160 mOhms-- 55 C+ 125 C235.6 GHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
LQG15HN15NG02D


15nH SMD,0.5x1mm Inductors (SMD) ROHS
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Murata 16425
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between Wed. 08 Jul to Fri. 10 Jul
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AUD 0.0445

Multiples of: 1

Multilayer Unshielded15 nH30 %400 mA450 mOhms-- 55 C+ 125 C82.3 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQW15AN4N7C80D


RF Inductors - SMD
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Murata 16425
Ships to you
between Wed. 08 Jul to Fri. 10 Jul
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AUD 0.1036

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded4.7 nH0.2 nH1.2 A71 mOhms-- 55 C+ 125 C318 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQW15AN3N9G8ZD


RF Inductors - SMD 3.9 NH 2%
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Murata 16393
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between Wed. 08 Jul to Fri. 10 Jul
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AUD 0.1138

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded3.9 nH2 %1.95 A30 mOhms-- 55 C+ 125 C1010 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQW15AN3N5G8ZD


RF Inductors - SMD
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Murata 16362
Ships to you
between Wed. 08 Jul to Fri. 10 Jul
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AUD 0.1474

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded3.5 nH2 %1.95 A30 mOhms-- 55 C+ 125 C3010 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
MLG1005S4N7STD25


RF Inductors - SMD IND 0402 4.7nH StdQ AEC Q200 RF IND
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TDK 16361
Ships to you
between Wed. 08 Jul to Fri. 10 Jul
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AUD 0.0815

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded4.7 nH0.3 nH700 mA250 mOhms-- 55 C+ 125 C85.4 GHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
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