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
  
                         
LQW2UASR22G00L


220nH ±2% 840mO 1008 Inductors (SMD) ROHS
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Murata 3656
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.1552

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Wirewound1008 (2520 METRIC)Unshielded220 nH2 %500 mA840 mOhms-- 55 C+ 125 C45700 MHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
LQW18AN8N7C80D


RF Inductors - SMD
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Murata 3655
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.1312

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded8.7 nH0.2 nH1.6 A52 mOhms-- 55 C+ 125 C384.75 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
LQP03TN82NJ02D


RF Inductors - SMD 82 NH 5%
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Murata 3654
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.0207

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Thin Film0201 (0603 METRIC)Unshielded82 nH5 %100 mA10 Ohms-- 55 C+ 125 C81 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQW18AN6N2D0ZD


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 3652
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.1086

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded6.2 nH0.5 nH750 mA82 mOhms-- 55 C+ 125 C356 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
L06032R2BGSTR


RF Inductors - SMD 2.2nH 1000mA 0603 DC =0.08ohm
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Kyocera AVX 3650
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.6019

Multiples of: 1

 0603 (1608 METRIC)Unshielded2.2 nH0.1 nH1 A80 mOhms - 55 C+ 125 C2010 GHzStandard1.6 mm0.81 mm0.61 mm   0603, 0805Reel , Cut Tape
L0805150JEWTR


RF Inductors - SMD 15nH 5%
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Kyocera AVX 3650
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 1.0309

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Thin Film0805 (2012 METRIC)Unshielded15 nH5 %1 A200 mOhms-- 55 C+ 125 C362.2 GHzStandard2.11 mm1.5 mm0.91 mm-  0603, 0805Reel , Cut Tape
L08052R2CEWTR


RF Inductors - SMD 2.2nH
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Kyocera AVX 3647
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.6785

Multiples of: 1

Thin Film0805 (2012 METRIC)Unshielded2.2 nH0.2 nH2 A70 mOhms-- 55 C+ 125 C4210 GHzStandard2.11 mm1.5 mm0.91 mm-  0603, 0805Reel , Cut Tape
MLF1608DR68KTA00


Inductor RF Chip Shielded Multi-Layer 680nH 10% 25MHz 15Q-Factor Ferrite 70mA 1.25Ohm DCR 0603 T/R
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TDK 3608
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between Fri. 24 Jul to Wed. 29 Jul
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AUD 0.0368

Multiples of: 20

Multilayer0603 (1608 METRIC)Shielded680 nH10 %70 mA1.25 Ohms-- 55 C+ 125 C15210 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
NLV25T-180J-EF


RF Inductors - SMD 18uH 4.8ohms 130mA Wound Ferrite
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TDK 3346
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between Fri. 24 Jul to Wed. 29 Jul
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AUD 0.0434

Multiples of: 10

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded18 uH5 %130 mA4.8 Ohms-- 40 C+ 105 C2524 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
NLCV32T-3R3M-EFD


RF Inductors - SMD 3.3uH 0.16ohms 690mA 3.2x2.5mm AEC-Q200
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TDK 1712
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between Thu. 16 Jul to Mon. 20 Jul
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AUD 0.1638

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Wirewound1210 (3225 METRIC)Unshielded3.3 uH20 %690 mA160 mOhms-- 40 C+ 105 C1054 MHzStandard3.2 mm2.5 mm2.4 mm-FerriteAEC - Q200NLCV25 - EFDReel , Cut Tape
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