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
  
                         
MLF1608A1R2JTD25


RF Inductors - SMD 1.2uH 650mohms 50mA +/-5% Fer AEC-Q200
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TDK 5591
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AUD 0.1577
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Multilayer0603 (1608 METRIC)Shielded1.2 uH5 %50 mA650 mOhms-- 55 C+ 125 C35150 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
CW160808-22NJ


Inductor RF Wirewound 0.022uH 5% 250MHz 35Q-Factor Alumina 0.7A 0.19Ohm DCR 0603 T/R
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Bourns 5590
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AUD 0.0819
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Wirewound0603 (1608 METRIC)Unshielded22 nH5 %700 mA190 mOhms-- 40 C+ 125 C353 GHzStandard1.65 mm1.05 mm1 mm-Ceramic CW160808Reel , Cut Tape
LQW03AW6N8J00D


RF Inductors - SMD 6.8 NH +/-5%
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Murata 5587
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AUD 0.1631
Multiples of: 5

Wirewound0201 (0603 METRIC)Unshielded6.8 nH5 %460 mA240 mOhms-- 55 C+ 125 C417.7 GHzStandard0.53 mm0.4 mm0.4 mm-  LQWReel , Cut Tape
LQW15AN82NG0ZD


RF Inductors - SMD
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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.

Murata 5586
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AUD 0.1232
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Wirewound0402 (1005 METRIC)Unshielded82 nH2 %130 mA2.24 Ohms-- 55 C+ 125 C202.3 GHzStandard1 mm0.5 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
AIML-0805-270K-T


RF Inductors - SMD FIXED IND 27UH 5MA 1.15 OHM SMD
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ABRACON 5585
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AUD 0.0971
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Multilayer Ferrite Chip Inductor0805 (2012 METRIC)Shielded27 uH10 %5 mA1.15 Ohms - 55 C+ 125 C3014 MHzStandard2 mm1.25 mm1.25 mm Ferrite AIML - 0805Reel , Cut Tape
CW201212-R47J


Inductor RF Wirewound 0.47uH 5% 50MHz 33Q-Factor Ferrite 0.25A 1.76Ohm DCR 0805 T/R
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Bourns 5580
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AUD 0.1851
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Wirewound0805 (2012 METRIC)Unshielded470 nH5 %250 mA1.72 Ohms-- 40 C+ 125 C33375 MHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW201212Reel , Cut Tape
AIMC-0603-R18J-T


RF Inductors - SMD FIXED IND 180NH 300MA 1.8 OHM
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ABRACON 5578
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AUD 0.0696
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Multilayer Ceramic Chip Inductor0603 (1608 METRIC)Shielded180 nH5 %200 mA1.9 Ohms - 55 C+ 125 C15400 MHzStandard1.6 mm0.8 mm0.8 mm Ceramic AIMC - 0603Reel , Cut Tape
B82422A3680K100


RF Inductors - SMD 68nH 480mA 10% 1210 SMD, AEC-Q200
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TDK 5566
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AUD 0.3736
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Wirewound1210 (3225 METRIC)Unshielded68 nH10 %480 mA210 mOhms-- 55 C+ 145 C271.15 GHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422AReel , Cut Tape
MLG1005S2N2STD25


RF Inductors - SMD IND 0402 2.2nH StdQ AEC Q200 RF IND
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TDK 5559
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AUD 0.0852
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Multilayer0402 (1005 METRIC)Unshielded2.2 nH0.3 nH900 mA150 mOhms-- 55 C+ 125 C78.6 GHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
B82422A3561K100


RF Inductors - SMD SMT-INDUCTOR 1210 0.56UH 10%, AECQ200
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TDK 3645
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AUD 0.3043
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Wirewound1210 (3225 METRIC)Unshielded560 nH10 %150 mA2.2 Ohms-- 55 C+ 145 C22400 MHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422AReel , Cut Tape
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