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
  
                         
0402AF-561XJLW


RF Inductors - SMD 1005 560nH Unshld 5% 200mA 920mOhms
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Coilcraft 0
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AUD 0.859

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded560 nH5 %200 mA920 mOhms-- 40 C+ 85 C-600 MHzStandard1.12 mm0.66 mm0.66 mm-Ferrite 0402AFReel , Cut Tape
0603CT-3N0XJRW


RF Inductors - SMD 0603 3nH Unshld 5% 1.6A 39mOhms
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AUD 0.8636

Multiples of: 1

Wirewound Unshielded3 nH5 %1.6 A39 mOhms-- 40 C+ 125 C-10.7 GHzStandard1.63 mm0.84 mm0.61 mm-Ceramic 0603CTReel , Cut Tape
1812SMS-39NGLC


RF Inductors - SMD 1812 39nH Unshld 2% 3A 4.4mOhms AECQ2
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AUD 0.8683

Multiples of: 1

Wirewound1812 (4532 METRIC)Unshielded39 nH2 %3 A4.4 mOhms-- 40 C+ 125 C1002.1 GHzStandard6.35 mm4.95 mm4.2 mm-AirAEC - Q2001812SMSReel , Cut Tape
PM105-390M-RC


RF Inductors - SMD 39uH 20%
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Bourns 0
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AUD 0.8892

Multiples of: 1

Smd Power Inductor Unshielded39 uH20 %520 mA160 mOhms - 30 C+ 100 C 12 MHz   5.8 mm9.8 mm  Pm105Reel
AL05B05N6GTR


RF Inductors - SMD 5.6nH 2% AIR CORE
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AUD 0.8913

Multiples of: 1

Toroidal Unshielded5.6 nH2 %1.6 A9 mOhms - 40 C+ 125 C10010 GHzStandard4.04 mm1.42 mm1.37 mm Air ALReel
AL05B7N15GTR


RF Inductors - SMD 7.15nH 2% Air Core
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AUD 0.8913

Multiples of: 1

Toroidal Unshielded7.15 nH2 %1.6 A10 mOhms - 40 C+ 125 C1006 GHzStandard4.04 mm1.42 mm1.37 mm Air ALReel
0603DC-R47XJRW


RF Inductors - SMD 0603 470nH 70mA 5% DCR=5.4Ohms AEC-Q200
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AUD 0.9109

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded470 nH5 %220 mA5.4 Ohms-- 40 C+ 125 C-600 MHzStandard1.7 mm0.99 mm0.89 mm-CeramicAEC - Q2000603DCReel , Cut Tape
0908SQ-8N1GLC


RF Inductors - SMD 8.1nH Unshld 2% 4.4A 6mOhms
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AUD 0.9261

Multiples of: 1

Wirewound2.134 mm x 1.829 mm x 1.473 mmUnshielded8.1 nH2 %4.4 A6 mOhms-- 40 C+ 125 C1305.2 GHzStandard1.473 mm2.134 mm1.829 mm-Air 090xSQReel , Cut Tape
0402DC-10NXJRW


RF Inductors - SMD 1005 10nH Unshld 5% 1.5A 73mOhms
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AUD 0.9306

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded10 nH5 %1.5 A73 mOhms-- 40 C+ 125 C1487.39 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
0402DC-27NXJRW


RF Inductors - SMD 1005 27nH Unshld 5% 920mA 192.9mOhms
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AUD 0.9319

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded27 nH5 %920 mA192.9 mOhms-- 40 C+ 125 C714.52 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
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