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
  
                         
NLV25T-1R2J-EF


RF Inductors - SMD 1.2uH 1.2ohms 230mA Wound Ferrite
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TDK 3676
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0522

Multiples of: 10

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded1.2 uH5 %230 mA1.2 Ohms-- 40 C+ 105 C30230 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
0603AQC-010J-01


RF Inductors - SMD Wire-wound Ceramic Chip Inductor AEC-Q200
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Fastron 3671
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2438

Multiples of: 1

Chip Inductor0603 (1608 METRIC)Unshielded10 nH5 %2.7 A50 mOhms - 40 C+ 140 C453.85 GHzStandard1.7 mm1.12 mm1.05 mm CeramicAEC - Q2000603AQCReel , Cut Tape
AIMC-0603-R22J-T


RF Inductors - SMD FIXED IND 220NH 300MA 2.1 OHM
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ABRACON 3670
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0733

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Multilayer Ceramic Chip Inductor0603 (1608 METRIC)Shielded220 nH5 %200 mA2.4 Ohms - 55 C+ 125 C15350 MHzStandard1.6 mm0.8 mm0.8 mm Ceramic AIMC - 0603Reel , Cut Tape
LQW2BASR68J00L


RF Inductors - SMD 680 NH 5%
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Murata 3668
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.11

Multiples of: 1

Wirewound0805 (2015 METRIC)Unshielded680 nH5 %190 mA2.2 Ohms-- 55 C+ 125 C23250 MHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
LQW18CA85NJ00D


RF Inductors - SMD Fixed IND 85nH 1650mA NONAUTO
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Murata 3666
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3381

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded85 nH5 %1.65 A48 mOhms-- 55 C+ 125 C331.8 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQW2UASR39G00L


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 3664
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1857

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded390 nH2 %470 mA1.12 Ohms-- 55 C+ 125 C45500 MHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
MCL2012V2-4R7-R


RF Inductors - SMD 4.7 NH 20%
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Eaton 3662
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0384

Multiples of: 1

Multilayer0805 (2012 METRIC)Unshielded4.7 nH5 %500 mA200 mOhms - 40 C+ 85 C   2 mm1.2 mm0.9 mm   MCLReel , Cut Tape
KLZ2012MHR4R7WTD25


RF Inductors - SMD 4.7uH 2MHz 20% 2012 AEC-Q200
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TDK 3661
Ships to you
between Fri. 21 Nov to Thu. 27 Nov
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AUD 0.078

Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded4.7 uH20 %170 mA500 mOhms180 mA- 55 C+ 150 C--Flexible (Soft)2 mm1.25 mm0.85 mm-FerriteAEC - Q200KLZ - HRReel , Cut Tape
B82422H1102K


RF Inductors - SMD 1uH 1150mA 10% 3.2x2.5mm SMD
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TDK 3658
Ships to you
between Fri. 21 Nov to Thu. 27 Nov
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AUD 0.2475

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded1 uH10 %1.15 A100 mOhms1.835 A- 55 C+ 150 C8150 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200B82422HReel , Cut Tape
LQW18AN9N5D00D


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 3637
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0592

Multiples of: 10

Wirewound0603 (1608 METRIC)Unshielded9.5 nH0.5 nH650 mA110 mOhms-- 55 C+ 125 C356 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
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