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
  
                         
IWC0402D33NR-3G


RF Inductors - SMD 0402 33nH 2% 400mA
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Laird Performance Materials 19400
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USD 0.0873
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Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded33 nH2 %400 mA450 mOhms-- 40 C+ 125 C242.35 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
IWC0402D27NR-3G


RF Inductors - SMD 0402 27nH 2% 400mA
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Laird Performance Materials 19400
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USD 0.0884
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Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded27 nH2 %400 mA400 mOhms-- 40 C+ 125 C242.48 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
IWC0402AR10R-3G


RF Inductors - SMD 0402 100nH 2% 30mA
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Laird Performance Materials 19400
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USD 0.0884
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Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded100 nH2 %30 mA2 Ohms-- 40 C+ 125 C201.16 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
IWC0402A68NR-3G


RF Inductors - SMD 0402 68nH 2% 100mA
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Laird Performance Materials 19400
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USD 0.0884
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Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded68 nH2 %100 mA1.12 Ohms-- 40 C+ 125 C221.62 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
IWC0402AR12R-3G


RF Inductors - SMD 0402 120nH 2% 110mA
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Laird Performance Materials 19400
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USD 0.0884
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Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded120 nH2 %110 mA2.66 Ohms-- 40 C+ 125 C201 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
IWC0402A82NR-3G


RF Inductors - SMD 0402 82nH 2% 50mA
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Laird Performance Materials 19400
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USD 0.0884
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Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded82 nH2 %50 mA1.55 Ohms-- 40 C+ 125 C201.23 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
IWC0402B39NR-3G


RF Inductors - SMD 0402 39nH 2% 200mA
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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 19400
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USD 0.0884
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Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded39 nH2 %200 mA550 mOhms-- 40 C+ 125 C252.1 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
IWC0402A47NR-3G


RF Inductors - SMD 0402 47nH 2% 150mA
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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 19400
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USD 0.0884
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Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded47 nH2 %150 mA830 mOhms-- 40 C+ 125 C202.1 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
IWC0603F47NR-3G


RF Inductors - SMD 0603 47nH 2% 600mA
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Laird Performance Materials 19400
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USD 0.0965
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Wirewound1.8 mm x 1.12 mm x 1.02 mmUnshielded47 nH2 %600 mA280 mOhms-- 40 C+ 125 C382 GHzStandard1.8 mm1.12 mm1.02 mm-Ceramic IWC0603Reel , Cut Tape
IWC0603CR12R-3G


RF Inductors - SMD 0603 120nH 2% 300mA
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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 19400
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USD 0.0965
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Wirewound1.8 mm x 1.12 mm x 1.02 mmUnshielded120 nH2 %300 mA750 mOhms-- 40 C+ 125 C321.3 GHzStandard1.8 mm1.12 mm1.02 mm-Ceramic IWC0603Reel , Cut Tape
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