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
  
                         
PM1008-R39K-RC


RF Inductors - SMD 0.39uH 10%
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AUD 0.2017
Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded390 nH10 %470 mA1.12 Ohms-- 55 C+ 125 C45500 MHzStandard2.5 mm2 mm1.6 mm-Ceramic PM1008Reel , Cut Tape
L02011R2AHSTR\500


RF Inductors - SMD 1.2nH
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AUD 0.1896
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Thin Film0201 (0603 METRIC)Unshielded1.2 nH0.05 nH300 mA300 mOhms-- 55 C+ 125 C724 GHzStandard0.6 mm0.325 mm0.225 mm-  Accu - LReel , Cut Tape
L0201R82AHSTR


RF Inductors - SMD 0.82nH
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AUD 0.1899
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded820 pH0.05 nH400 mA200 mOhms-- 55 C+ 125 C828 GHzStandard0.6 mm0.325 mm0.225 mm-  Accu - LReel , Cut Tape
PM1008-R12K-RC


RF Inductors - SMD 0.12uH 10%
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AUD 0.2017
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 1008 (2520 METRIC)Unshielded120 nH10 %650 mA680 mOhms - 55 C+ 125 C60950 MHzStandard2.5 mm2 mm1.6 mm Ceramic PM1008Reel , Cut Tape
WCLA2012V1-4R7-R


RF Inductors - SMD WCLA Auto Chip IND 2012 4.7nH 2 Pads
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Eaton 0
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AUD 0.2052
Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded4.7 nH5 %600 mA50 mOhms-- 40 C+ 125 C406 GHzStandard2.3 mm1.7 mm1.52 mm- AEC - Q200WCLAReel , Cut Tape
5508 020 24 00


RF Inductors - SMD RF Chip Inductor SMD 2.7nH 0805 10% Tol
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Sumida 0
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AUD 0.1919
Multiples of: 1

 0805 (2012 METRIC)Unshielded2.7 nH10 %1 A30 mOhms - 55 C+ 125 C206 GHzStandard      5406Reel , Cut Tape
0603WL391GT


RF Inductors - SMD 390PF 2% 0603
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AUD 0.1946
Multiples of: 1

 0603 (1812 METRIC)          Standard      WLReel , Cut Tape
IWC0603AR27R-3G


RF Inductors - SMD 0603 270nH 2% 170mA
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AUD 0.2036
Multiples of: 1

Wirewound1.8 mm x 1.12 mm x 1.02 mmUnshielded270 nH2 %170 mA2.36 Ohms-- 40 C+ 125 C24900 MHzStandard1.8 mm1.12 mm1.02 mm-Ceramic IWC0603Reel , Cut Tape
IWC0603F27NR-3G


RF Inductors - SMD 0603 27nH 2% 600mA
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AUD 0.2036
Multiples of: 20000

Wirewound1.8 mm x 1.12 mm x 1.02 mmUnshielded27 nH2 %600 mA220 mOhms-- 40 C+ 125 C402.8 GHzStandard1.8 mm1.12 mm1.02 mm-Ceramic IWC0603Reel , Cut Tape
IWC0603BR22R-3G


RF Inductors - SMD 0603 220nH 2% 200mA
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Laird Performance Materials 0
6 to 16 Weeks Calender.png

AUD 0.2036
Multiples of: 20000

Wirewound1.8 mm x 1.12 mm x 1.02 mmUnshielded220 nH2 %200 mA2.02 Ohms-- 40 C+ 125 C25900 MHzStandard1.8 mm1.12 mm1.02 mm-Ceramic IWC0603Reel , Cut Tape
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