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
  
                         
NLV25T-R56J-EF


RF Inductors - SMD 560nH 750mohms 325mA Wound Ferrite
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TDK 1891
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AUD 0.0599
Multiples of: 10

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded560 nH5 %325 mA750 mOhms-- 40 C+ 105 C30325 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
PE-0603CLHR68STS


RF Inductors - SMD 0603 680nH 1050mA DCR=195mOhms RF
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Pulse 1852
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AUD 0.131
Multiples of: 1

Multilayer0603 (1608 METRIC)Shielded680 nH-1.05 A180 mOhms750 mA- 40 C+ 85 C-100 MHzStandard1.6 mm0.8 mm0.8 mm-Ceramic PE - 0603CLHReel , Cut Tape
NLCV25T-R47M-EFR


RF Inductors - SMD 470nH 96mohms 1.34A 125C Wound Ferrite
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TDK 1852
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AUD 0.1709
Multiples of: 5

Wirewound1008 (2520 METRIC)Unshielded470 nH20 %1.34 A80 mOhms-- 40 C+ 125 C5-Standard2.5 mm2 mm1.8 mm-Ferrite NLCV - EFRReel , Cut Tape
LQW2UASR75G00L


RF Inductors - SMD
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Murata 1844
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AUD 0.1877
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Wirewound1008 (2520 METRIC)Unshielded750 nH2 %360 mA1.54 Ohms-- 55 C+ 125 C45360 MHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
NLFV32T-4R7M-EF


RF Inductors - SMD 3.2mm x 2.5mm x 2.2mm, -40 to +105 degC, 360mA, 4.7?H, 156mohm
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TDK 1844
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AUD 0.2423
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Wirewound1210 (3225 METRIC)Shielded4.7 uH20 %360 mA130 mOhms-- 40 C+ 105 C--Standard3.2 mm2.5 mm2.2 mm-Ferrite NLFV32 - EFReel , Cut Tape
AL01656N0JTS


RF Inductors - SMD 56nH 5% AIR CORE
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Kyocera AVX 1843
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AUD 0.2423
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Wirewound3.81 mm x 4.2 mm x 4.83 mmUnshielded56 nH5 %3 A6.2 mOhms-- 40 C+ 125 C1001.5 GHzStandard4.83 mm3.81 mm4.2 mm-Air ALReel , Cut Tape
ISC1812ES2R7K


RF Inductors - SMD 2.7uh 10%
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Vishay 1843
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AUD 0.7048
Multiples of: 1

Molded1812 (4532 METRIC) 2.7 uH  820 mOhms     Standard      ISCReel , Cut Tape
AISC-Q0603HQ-12NG-T


RF Inductors - SMD IND 12nH 1.1A 88m?
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Abracon 1838
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AUD 0.1822
Multiples of: 1

Wirewound0603 (1812 METRIC)Unshielded12 nH2 %1.1 A88 mOhms - 40 C+ 125 C374.1 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - Q0603HQReel , Cut Tape
NLV25T-330J-EF


RF Inductors - SMD 33uH 7.1ohms 110mA Wound Ferrite
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TDK 1823
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AUD 0.0398
Multiples of: 10

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded33 uH5 %110 mA7.1 Ohms-- 40 C+ 105 C2520 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
IMC0805ER2R2J01


RF Inductors - SMD 2.2uH 5%
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Vishay 1119
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AUD 0.1966
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Wirewound0805 (2012 METRIC)Unshielded2.2 nH0.3 nH800 mA60 mOhms-- 40 C+ 125 C506 GHzStandard2 mm1.25 mm1.2 mm-Ceramic IMCReel , Cut Tape
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