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
  
                         
LQW15AN15NG8ZD


RF Inductors - SMD 15 NH 2%
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Murata 10733
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AUD 0.087
Multiples of: 5

Wirewound0402 (1005 METRIC)Shielded15 nH2 %1.15 A114 mOhms-- 55 C+ 125 C311.15 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
MLG0603P62NJT000


RF Inductors - SMD IND 0201 62nH Hi-Q SMD RF IND
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TDK 10718
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AUD 0.0223
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded62 nH5 %100 mA3.5 Ohms-- 55 C+ 125 C101.6 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
IWC0603F39NR-3G


RF Inductors - SMD 0603 39nH 2% 600mA
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Laird Performance Materials 10708
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AUD 0.1798
Multiples of: 1

Wirewound1.8 mm x 1.12 mm x 1.02 mmUnshielded39 nH2 %600 mA250 mOhms-- 40 C+ 125 C402.2 GHzStandard1.8 mm1.12 mm1.02 mm-Ceramic IWC0603Reel , Cut Tape
LQW18CNR27J0HD


RF Inductors - SMD 270nH 750mA AEC-Q200
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Murata 10677
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AUD 0.1508
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded270 nH5 %750 mA160 mOhms - 40 C+ 125 C 660 MHz 1.6 mm1.6 mm0.8 mm FerriteAEC - Q200LCQW18CNReel , Cut Tape
MCLA1005V2-1R0-R


RF Inductors - SMD MCLA Auto Chip IND 1005 1.0nH 2 Pads
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Eaton 10670
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AUD 0.0294
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded1 nH0.3 nH400 mA100 mOhms-- 40 C+ 125 C810 GHzStandard1 mm0.5 mm0.5 mm- AEC - Q200MCLAReel , Cut Tape
LQP03HQ1N5W02D


RF Inductors - SMD 1.5 NH 1A
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Murata 10670
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AUD 0.0728
Multiples of: 10

Thin Film0201 (0603 METRIC)Unshielded1.5 nH0.05 nH1 A50 mOhms-- 55 C+ 125 C2012 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
AIML-0805-R10K-T


RF Inductors - SMD FIXED IND 100NH 250MA 300 MOHM
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ABRACON 10670
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AUD 0.0934
Multiples of: 1

Multilayer Ferrite Chip Inductor0805 (2012 METRIC)Shielded100 nH10 %250 mA300 mOhms - 55 C+ 125 C20235 MHzStandard2 mm1.25 mm1.25 mm Ferrite AIML - 0805Reel , Cut Tape
PE-0603CD221JTT


RF Inductors - SMD SMD IND
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Pulse 10670
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AUD 0.1944
Multiples of: 1

Multilayer0603 (1608 METRIC)Unshielded220 nH5 %200 mA1.9 Ohms-- 40 C+ 125 C25900 MHzStandard1.8 mm1.24 mm1.02 mm-Ceramic CDReel , Cut Tape
MLG0603P5N6ST000


RF Inductors - SMD IND 0201 5.6nH Hi-Q SMD RF IND
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TDK 10661
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AUD 0.0276
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Multilayer0201 (0603 METRIC)Unshielded5.6 nH0.3 nH350 mA400 mOhms-- 55 C+ 125 C145.3 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
WCLA3225V1-2R2-R


RF Inductors - SMD Chip IND 2.2uH 0.88A SMT 2 Pad
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Eaton 10660
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AUD 0.288
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Wirewound1210 (3225 METRIC)Shielded2.2 uH10 %880 mA170 mOhms - 55 C+ 125 C10190 MHz 3.6 mm2.8 mm2.4 mm Ferrite WCLAReel , Cut Tape
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