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
  
                         
0402DC-6N2XJRW


RF Inductors - SMD 1005 6.2nH Unshld 5% 1.8A 57mOhms
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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.

Coilcraft 0
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AUD 0.9319

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded6.2 nH5 %1.8 A57 mOhms-- 40 C+ 125 C1469.2 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
0402DC-3N3XJRW


RF Inductors - SMD 1005 3.3nH Unshld 5% 2.1A 37mOhms
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Coilcraft 0
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AUD 0.9319

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded3.3 nH5 %2.1 A37 mOhms-- 40 C+ 125 C16014.24 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
0402DC-5N6XJRW


RF Inductors - SMD 1005 5.6nH Unshld 5% 1.8A 57mOhms
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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.

Coilcraft 0
6 to 16 Weeks Calender.png

AUD 0.9319

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded5.6 nH5 %1.8 A57 mOhms-- 40 C+ 125 C14611 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
0402DC-68NXJRW


RF Inductors - SMD 1005 68nH Unshld 5% 400mA 943mOhms
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AUD 0.9319

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded68 nH5 %400 mA943 mOhms-- 40 C+ 125 C542.8 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
0402DC-15NXJRW


RF Inductors - SMD 1005 15nH Unshld 5% 1.2A 115mOhms
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Coilcraft 0
6 to 16 Weeks Calender.png

AUD 0.9319

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded15 nH5 %1.2 A115 mOhms-- 40 C+ 125 C1106.2 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
0402DC-4N7XJRW


RF Inductors - SMD 1005 4.7nH Unshld 5% 1.85A 48mOhms
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AUD 0.9319

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded4.7 nH5 %1.85 A48 mOhms-- 40 C+ 125 C14612.7 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
0402HP-10NXJRW


RF Inductors - SMD 1005 10nH Unshld 5% 1.3A 85mOhms
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AUD 0.9358

Multiples of: 1

   10 nH                 
ISC1812EB100K


RF Inductors - SMD ISC-1812 10 10% EB E3
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Vishay 0
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AUD 0.7254

Multiples of: 1

Molded1812 (4532 METRIC)    820 mOhms     Standard      ISC1812Bulk
L0805180JEWTR


Inductor RF Chip Thin Film Multilayer 18nH 5% 450MHz 30Q-Factor Ceramic 1A 350mOhm DCR 0805 T/R
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Kyocera AVX 0
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AUD 0.9378

Multiples of: 1

Thin Film0805 (2012 METRIC)Unshielded18 nH5 %1 A350 mOhms-- 55 C+ 125 C301.7 GHzStandard2.11 mm1.5 mm0.91 mm-  0603, 0805Reel , Cut Tape
0402DC-8N2XJRW


RF Inductors - SMD 1005 8.2nH Unshld 5% 1.6A 70mOhms
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AUD 0.9542

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded8.2 nH5 %1.6 A70 mOhms-- 40 C+ 125 C1388.33 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
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