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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(Ex. GST)(▲▼)		Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
IWC1008DR39R-3G


RF Inductors - SMD 1008 390nH 2% 470mA
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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.

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AUD 0.2528
Multiples of: 10000

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
IWC1008ER27R-3G


RF Inductors - SMD 1008 270nH 2% 500mA
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AUD 0.2528
Multiples of: 10000

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
IWC1008J22NR-3G


RF Inductors - SMD 1008 22nH 2% 1000mA
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AUD 0.2528
Multiples of: 10000

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
IWC1008J68NR-3G


RF Inductors - SMD 1008 68nH 2% 1000mA
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AUD 0.2528
Multiples of: 10000

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
IWC1008DR82R-3G


RF Inductors - SMD 1008 820nH 2% 400mA
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AUD 0.2528
Multiples of: 10000

Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded820 nH2 %400 mA1.62 Ohms-- 40 C+ 125 C45350 MHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
IWC1008FR12R-3G


RF Inductors - SMD 1008 120nH 2% 650mA
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AUD 0.2528
Multiples of: 10000

Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded120 nH2 %650 mA -- 40 C+ 125 C60950 MHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
IWC1008FR18R-3G


RF Inductors - SMD 1008 180nH 2% 620mA
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AUD 0.2528
Multiples of: 10000

Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded180 nH2 %650 mA770 mOhms-- 40 C+ 125 C45750 MHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
IWC1008J33NR-3G


RF Inductors - SMD 1008 33nH 2% 1000mA
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AUD 0.2528
Multiples of: 10000

Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded33 nH2 %1 A140 mOhms-- 40 C+ 125 C601.6 GHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
IWC1008J82NR-3G


RF Inductors - SMD 1008 82nH 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.

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AUD 0.2528
Multiples of: 10000

Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded82 nH2 %1 A220 mOhms-- 40 C+ 125 C601 GHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
IWC1008DR47R-3G


RF Inductors - SMD 1008 470nH 2% 470mA
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AUD 0.2528
Multiples of: 10000

Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded470 nH2 %470 mA1.19 Ohms-- 40 C+ 125 C45450 MHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
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