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
  
                         
LCCI0603J82NGTAR


RF Inductors - SMD 82nH Tol 5% 0603 300 mA DCR=0.95 Ohms
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Kyocera AVX 3880
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AUD 0.0505
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Multilayer0603 (1608 METRIC)Unshielded82 nH5 %300 mA950 mOhms-- 40 C+ 85 C12600 MHzStandard1.6 mm0.8 mm0.8 mm-  LCCIReel , Cut Tape
AIML-0603-180K-T


RF Inductors - SMD FIXED IND 18UH 1MA 1.85 OHM SMD
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ABRACON 3880
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AUD 0.0646
Multiples of: 4000

Multilayer0603 (1608 METRIC)Shielded18 uH10 %1 mA1.85 Ohms - 55 C+ 125 C2018 MHzStandard1.6 mm0.8 mm0.8 mm Ferrite AIML - 0603Reel , Cut Tape
MLF2012DR18MT000


RF Inductors - SMD 2mm x 1.25mm x 0.85mm, -55 to +125 degC, 300mA, 0.18?H, 250mohm
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TDK 3880
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AUD 0.0757
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Multilayer0805 (2012 METRIC)Shielded180 nH20 %300 mA250 mOhms - 55 C+ 125 C20370 MHzStandard2 mm1.25 mm10.5 mm Ferrite MLFReel , Cut Tape
LQW18AS12NJ00D


RF Inductors - SMD
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Murata 3880
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AUD 0.0785
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Wirewound0603 (1608 METRIC)Unshielded12 nH5 %700 mA130 mOhms-- 40 C+ 125 C354 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQW18ASR33G00D


RF Inductors - SMD
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Murata 3880
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AUD 0.0824
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded330 nH2 %100 mA3.89 Ohms - 40 C+ 125 C25900 MHzStandard1.6 mm0.8 mm0.8 mm   LQWReel , Cut Tape
BWCS0012070710NG00


RF Inductors - SMD 10nH RDC=0.20Ohms 480mA
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Pulse 3880
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AUD 0.0827
Multiples of: 4000

 1.6 mm x 0.7 mm x 0.66 mmUnshielded10 nH2 %480 mA200 mOhms480 mA- 40 C+ 125 C213.9 GHzStandard1.2 mm0.7 mm0.66 mm Ceramic BWCSReel , Cut Tape
LQW18ASR27J00D


RF Inductors - SMD
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Murata 3880
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AUD 0.0836
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded270 nH5 %170 mA2.3 Ohms-- 40 C+ 125 C24900 MHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQW18ASR39J00D


RF Inductors - SMD
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Murata 3880
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AUD 0.0843
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded390 nH5 %100 mA4.35 Ohms-- 40 C+ 125 C25900 MHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQW18AS56NG00D


RF Inductors - SMD
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Murata 3880
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AUD 0.0855
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Wirewound0603 (1608 METRIC)Unshielded56 nH2 %600 mA310 mOhms-- 40 C+ 125 C381.9 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
NLV25T-1R5J-EF


RF Inductors - SMD 1.5uH 1.3ohms 220mA Wound Ferrite
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TDK 3860
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AUD 0.0533
Multiples of: 10

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded1.5 uH5 %220 mA1.3 Ohms-- 40 C+ 105 C30182 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
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