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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Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
LQW2UASR18F00L


RF Inductors - SMD
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 1930
Ships to you
between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.3144

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded180 nH1 %620 mA770 mOhms-- 55 C+ 125 C45750 MHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
IMC1210ER33NK


RF Inductors - SMD 33uh 10%
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Vishay 1928
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between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.5372

Multiples of: 1

Molded1210 (3225 METRIC) 33 nH  15 mOhms     Standard      IMCReel , Cut Tape
1210R-682J


RF Inductors - SMD 6.8uH 5%
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API Delevan 1928
Ships to you
between Fri. 17 Jul to Tue. 21 Jul
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AUD 2.3221

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded6.8 uH5 %321 mA1.8 Ohms-- 55 C+ 125 C3040 MHzStandard3.51 mm2.67 mm2.57 mm-Ferrite 1210/RReel , Cut Tape
0805AS-R62J-08


Wire-wound Ceramic RF Chip
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Fastron 1926
Ships to you
between Mon. 13 Jul to Fri. 17 Jul
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AUD 0.2437

Multiples of: 1

                     
LQW18AS3N3G0CD


RF Inductors - SMD
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 1924
Ships to you
between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.34

Multiples of: 1

Multilayer Unshielded3.3 nH2 %700 mA45 mOhms-- 40 C+ 85 C355.9 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
PE-0805CD151GTT


RF Inductors - SMD SMD IND
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Pulse 1920
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between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.2465

Multiples of: 1

Multilayer0805 (2012 METRIC)Unshielded149.4 nH2 %400 mA560 mOhms-- 40 C+ 125 C50920 MHzStandard2.29 mm1.68 mm1.58 mm-Ceramic CDReel , Cut Tape
PM1008-2R2K-RC


Ind Chip Wirewound 2.2uH 10% 7.9MHz 25Q-Factor Ferrite 250mA 1008 T/R
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Bourns 1919
Ships to you
between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.1948

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded2.2 uH10 %290 mA2.8 Ohms-- 55 C+ 125 C28160 MHzStandard2.5 mm2 mm1.6 mm-Ceramic PM1008Reel , Cut Tape
LQG15WH16NG02D


RF Inductors - SMD Fixed IND 16nH 260mA POWRTRN
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Murata 1875
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between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.1345

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded16 nH2 %260 mA800 mOhms-- 55 C+ 125 C202.3 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
NLV32T-R22J-EF


RF Inductors - SMD 220nH 320mohms 450mA Wound Ferrite
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TDK 1687
Ships to you
between Mon. 27 Jul to Thu. 30 Jul
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AUD 0.0478

Multiples of: 10

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded220 nH5 %450 mA320 mOhms-- 40 C+ 105 C30350 MHzStandard3.2 mm2.5 mm2.2 mm Ferrite NLV32 - EFReel , Cut Tape
NLV25T-150J-EF


RF Inductors - SMD 15uH 4.4ohms 140mA Wound Ferrite
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TDK 467
Ships to you
between Fri. 17 Jul to Tue. 21 Jul
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AUD 0.1396

Multiples of: 1

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded15 uH5 %140 mA4.4 Ohms-- 40 C+ 105 C2526 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
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