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
  
                         
LQG15HZR27J02D


RF Inductors - SMD
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Murata 11594
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AUD 0.0551
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Multilayer0402 (1005 METRIC)Unshielded270 nH5 %110 mA4.94 Ohms-- 55 C+ 125 C8400 MHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
CIGT201610LHR47MNE


RF Inductors - SMD CIGT,Thin Film,0806,0.47uH,1.0?,7 embossed,-20 20%
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Samsung 1900
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AUD 0.1034
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Thin Film  470 nH20 %              CIGTReel , Cut Tape
LQP03TQ1N2B02D


RF Inductors - SMD 1.2nH 800mA 0201 (0603 metric) SUGGESTED ALT LQP03HQ1N2B02D
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Murata 1897
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AUD 0.0276
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Thin Film0201 (0603 METRIC)Unshielded1.2 nH0.1 nH800 mA80 mOhms-- 55 C+ 125 C1717 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
AISC-1008-2R7J-T


RF Inductors - SMD FIXED IND 2.7UH 290MA 3.2 OHM
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ABRACON 1896
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AUD 0.2894
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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
MCLA2012V1-6R8-R


RF Inductors - SMD MCLA Auto Chip IND 2012 6.8uH 2 Pads
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Eaton 1892
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AUD 0.0604
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Multilayer0805 (2012 METRIC)Unshielded6.8 uH10 %15 mA1.05 Ohms-- 40 C+ 125 C3029 MHzStandard2 mm1.2 mm0.9 mm- AEC - Q200MCLAReel , Cut Tape
ISC1210ER3R9K


RF Inductors - SMD 3.9uh 10%
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Vishay 1891
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AUD 1.1575
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Molded1210 (3225 METRIC) 3.9 uH10 %250 mA1.2 Ohms - 55 C+ 125 C3058 MHzStandard      ISCReel , Cut Tape
L02011R5BHSTR\500


RF Inductors - SMD 1.5nH
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Kyocera AVX 1890
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AUD 0.1966
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Thin Film0201 (0603 METRIC)Unshielded1.5 nH0.1 nH250 mA500 mOhms-- 55 C+ 125 C723 GHzStandard0.6 mm0.325 mm0.225 mm-  Accu - LReel , Cut Tape
MLF2012C150MT000


RF Inductors - SMD 15 UH 20%
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TDK 1889
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AUD 0.0844
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Multilayer0805 (2012 METRIC)Shielded15 uH20 %5 mA700 mOhms-- 55 C+ 125 C3040 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
NLV32T-3R3J-EF


RF Inductors - SMD 3.3uH 1.2ohms 260A Wound Ferrite
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TDK 504
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AUD 0.0626
Multiples of: 10

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded3.3 uH5 %260 mA1.2 Ohms-- 40 C+ 105 C3060 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
LQW2BASR22G00L


RF Inductors - SMD
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Murata 111
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AUD 0.1293
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Wirewound0805 (2015 METRIC)Unshielded220 nH2 %400 mA700 mOhms-- 55 C+ 125 C50820 MHzStandard2.09 mm1.53 mm1.42 mm-- LQW2BAReel , Cut Tape
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