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
  
                         
B82422A3681K100


RF Inductors - SMD 680nH 145mA 10% 1210 SMD, AEC-Q200
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TDK 1903
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AUD 0.3006
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Wirewound1210 (3225 METRIC)Unshielded680 nH10 %145 mA2.4 Ohms-- 55 C+ 145 C22280 MHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422AReel , Cut Tape
LQG15HS47NG02D


RF Inductors - SMD 47 NH 2% NH
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Murata 1901
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AUD 0.0436
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded47 nH2 %300 mA720 mOhms-- 55 C+ 125 C81 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LBM2016T820J


RF Inductors - SMD 963-LSQMB201616T820J RPLCMT PN 0806 82uH 10.01Ohms 5% 85mA
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Taiyo Yuden 1901
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AUD 0.091
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Wirewound0806 (2016 METRIC)Unshielded82 uH5 %85 mA10.01 Ohms-- 40 C+ 105 C2010 MHzStandard2 mm1.6 mm1.8 mm-  LBMReel , Cut Tape
AISC-0402-9N0J-T


RF Inductors - SMD FIXED IND 9NH 680MA 100 MOHM SMD
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ABRACON 1901
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AUD 0.1614
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Smd Ceramic Wire - Wound Chip Inductors0402 (1005 METRIC)Unshielded9 nH5 %680 mA100 mOhms - 40 C+ 125 C254160 MHz     Ceramic Aisc - 0402Reel
MLF2012K390MT000


RF Inductors - SMD 2mm x 1.25mm x 1.25mm, -40 to +85 degC, 4mA, 39?H, 2.4ohm
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TDK 1898
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AUD 0.08
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Multilayer0805 (2012 METRIC)Shielded39 uH20 %4 mA2.4 Ohms-- 55 C+ 125 C3523 MHzStandard2 mm1.25 mm1.25 mm Ferrite MLFReel , Cut Tape
AISC-1008-2R7J-T


RF Inductors - SMD FIXED IND 2.7UH 290MA 3.2 OHM
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ABRACON 1898
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AUD 0.2876
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Wirewound1008 (2520 METRIC)Unshielded2.7 uH5 %290 mA3.2 Ohms - 40 C+ 125 C2290 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
CC453232-391KL


RF Inductors - SMD 390uH 10% 796KHz
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Bourns 1896
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AUD 0.221
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Wirewound1812 (4532 METRIC) 390 uH10 %85 mA14 Ohms - 40 C+ 125 C203 MHzStandard4.2 mm3.2 mm3.2 mm   CC453232Reel , Cut Tape
LQW18CAR16J00D


RF Inductors - SMD Fixed IND 160nH 1300mA NONAUTO
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Murata 1896
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AUD 0.3381
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Wirewound0603 (1608 METRIC)Unshielded160 nH5 %1.3 A75 mOhms-- 55 C+ 125 C331.35 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
MLF2012K470KTD25


RF Inductors - SMD 47uH 2.7ohms 4mA +/-10% Fer AEC-Q200
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TDK 1891
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AUD 0.081
Multiples of: 10

Multilayer0805 (2012 METRIC)Shielded47 uH10 %4 mA2.7 Ohms-- 55 C+ 125 C3520 MHzStandard2 mm1.25 mm1.25 mm-FerriteAEC - Q200MLFReel , Cut Tape
B82422H1332K


RF Inductors - SMD 3.3uH 770mA 10% 3.2x2.5mm SMD
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TDK 1891
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AUD 0.3556
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Wirewound1210 (3225 METRIC)Unshielded3.3 uH10 %790 mA180 mOhms1.15 A- 55 C+ 150 C870 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200B82422HReel , Cut Tape
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