About RF inductors - SMD

Laird Performance Materials 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.

RF inductors - SMD

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(Ex. GST)(▲▼)		Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
IWC1008J68NR-3G


RF Inductors - SMD 1008 68nH 2% 1000mA
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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.

Laird Performance Materials Availability : 9700
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USD 0.12
Multiples of: 1

Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded68 nH2 %1 A200 mOhms-- 40 C+ 125 C651.3 GHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
IWC1008DR39R-3G


RF Inductors - SMD 1008 390nH 2% 470mA
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Laird Performance Materials Availability : 9700
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USD 0.12
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Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded390 nH2 %470 mA1.12 Ohms-- 40 C+ 125 C45500 MHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
IWC1008J39NR-3G


RF Inductors - SMD 1008 39nH 2% 1000mA
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USD 0.12
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Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded39 nH2 %1 A150 mOhms-- 40 C+ 125 C601.5 GHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
IWC1008J27NR-3G


RF Inductors - SMD 1008 27nH 2% 1000mA
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USD 0.12
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Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded27 nH2 %1 A130 mOhms-- 40 C+ 125 C551.6 GHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
IWC1008ER27R-3G


RF Inductors - SMD 1008 270nH 2% 500mA
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Laird Performance Materials Availability : 9700
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USD 0.12
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Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded270 nH2 %500 mA910 mOhms-- 40 C+ 125 C45600 MHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
IWC1008FR10R-3G


RF Inductors - SMD 1008 100nH 2% 650mA
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Laird Performance Materials Availability : 9700
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USD 0.12
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Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded100 nH2 %650 mA560 mOhms-- 40 C+ 125 C601 GHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
IWC1008J22NR-3G


RF Inductors - SMD 1008 22nH 2% 1000mA
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Laird Performance Materials Availability : 9700
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USD 0.12
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Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded22 nH2 %1 A120 mOhms-- 40 C+ 125 C552.4 GHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
IWC0805D82NR-3G


RF Inductors - SMD 0805 82nH 2% 400mA
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Laird Performance Materials Availability : 9690
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USD 0.1044
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Wirewound2.35 mm x 1.73 mm x 1.52 mmUnshielded82 nH2 %400 mA420 mOhms-- 40 C+ 125 C651.3 GHzStandard2.35 mm1.73 mm1.52 mm-Ceramic IWC0805Reel , Cut Tape
IWC0805DR10R-3G


RF Inductors - SMD 0805 100nH 2% 400mA
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Laird Performance Materials Availability : 9680
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USD 0.1044
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Wirewound2.35 mm x 1.73 mm x 1.52 mmUnshielded100 nH2 %400 mA460 mOhms-- 40 C+ 125 C651.2 GHzStandard2.35 mm1.73 mm1.52 mm-Ceramic IWC0805Reel , Cut Tape
IWC1008DR68R-3G


RF Inductors - SMD 1008 680nH 2% 400mA
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Laird Performance Materials Availability : 1938
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USD 0.1234
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Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded680 nH2 %400 mA1.47 Ohms-- 40 C+ 125 C45375 MHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
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