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
  
                         
PM1210-1R2J-RC


1.2 µH Unshielded Drum Core, Wirewound Inductor 215 mA 750mOhm Max 1210 (3225 Metric)
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Bourns 2072
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AUD 0.242
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Wirewound1210 (3225 METRIC)Unshielded1.2 uH5 %390 mA750 mOhms-- 55 C+ 105 C30100 MHzStandard2.9 mm2.5 mm2.2 mm-Ferrite PM1210Reel , Cut Tape
AISC-1206-39NJ-T


RF Inductors - SMD FIXED IND 39NH 1A 120 MOHM SMD
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ABRACON 2068
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AUD 0.4602
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Ceramic Wirewound RF Inductor1206 (3216 METRIC)Unshielded39 nH5 %1 A120 mOhms - 40 C+ 125 C501.8 GHzStandard3.56 mm2.16 mm1.52 mm Ceramic AISC - 1206Reel , Cut Tape
NLV32T-3R3J-EF


RF Inductors - SMD 3.3uH 1.2ohms 260A Wound Ferrite
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TDK 2066
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AUD 0.056
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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
LBM2016TR18J


RF Inductors - SMD 963-LSQMB201616TR18J RPLCMT PN 0806 .18uH 195mOhms 5% 560mA
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Taiyo Yuden 2066
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AUD 0.1027
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Wirewound0806 (2016 METRIC)Unshielded180 nH5 %560 mA195 mOhms-- 40 C+ 105 C30500 MHzStandard2 mm1.6 mm1.8 mm-  LBMReel , Cut Tape
CC453232-1R2KL


RF Inductors - SMD 1.2uH 10% 7.96MHz
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Bourns 2064
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AUD 0.2236
Multiples of: 1

Wirewound1812 (4532 METRIC)Unshielded1.2 uH10 %1 A120 mOhms-- 40 C+ 125 C10160 MHzStandard4.2 mm3.2 mm3.2 mm-Ferrite CC453232Reel , Cut Tape
AISC-0402-47NJ-T


RF Inductors - SMD FIXED IND 47NH 150MA 750 MOHM
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ABRACON 2061
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AUD 0.0335
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Wirewound0402 (1005 METRIC) 47 nH5 %150 mA750 mOhms - 25 C+ 85 C202.1 GHz-1.19 mm0.64 mm0.66 mm Ceramic Aisc - 0402Cut Tape
NLV32T-271J-EF


RF Inductors - SMD 270uH 28ohms 45mA Wound Ferrite
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TDK 2056
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AUD 0.0572
Multiples of: 10

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded270 uH5 %45 mA28 Ohms-- 40 C+ 105 C206 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
S1812R-104K


RF Inductors - SMD 100uH 10%
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API Delevan 2056
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AUD 4.1193
Multiples of: 1

RF Choke1812 (4532 METRIC)Shielded100 uH10 %169 mA7 Ohms-- 55 C+ 125 C407 MHzStandard4.8 mm3.4 mm3.4 mm-Ferrite S1812/RReel , Cut Tape
MLF1608A1R8KTA00


50mA 1.8uH ±10% 350mO 0603 Inductors (SMD) ROHS
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TDK 2017
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AUD 0.0459
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Multilayer0603 (1608 METRIC)Shielded1.8 uH10 %50 mA850 mOhms-- 55 C+ 125 C35130 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
LQW15AN16NH00D


RF Inductors - SMD 16 NH
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Murata 1571
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AUD 0.0297
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Wirewound0402 (1005 METRIC)Unshielded16 nH3 %370 mA240 mOhms-- 55 C+ 125 C254.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
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