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
  
                         
B82422T1332J000


RF Inductors - SMD SMT-INDUCTOR 1210 3.3UH 5%, AEC-Q200
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TDK 4848
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between Thu. 23 Jul to Mon. 27 Jul
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AUD 0.2707

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded3.3 uH5 %260 mA1.2 Ohms-- 55 C+ 125 C3060 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422TReel , Cut Tape
1206AS-R33J-01


RF Inductors - SMD Wire-wound Ceramic RF Chip Inductor
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Fastron 0
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AUD 0.2707

Multiples of: 2000

Wirewound1206 (3216 METRIC)Unshielded330 nH5 %590 mA620 mOhms     Standard    CeramicAEC - Q2001206ASReel
0805AS-6N8K-08


RF Inductors - SMD Wire-wound Ceramic RF Chip Inductor
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Fastron 0
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AUD 0.2567

Multiples of: 1000

Wirewound0805 (2012 METRIC)Unshielded6.8 nH10 %600 mA110 mOhms - 40 C+ 150 C505.5 GHzStandard2.3 mm1.8 mm1.6 mm CeramicAEC - Q2000805ASReel
0805AS-R10J-08


RF Inductors - SMD Wire-wound Ceramic RF Chip Inductor
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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.

Fastron 0
6 to 16 Weeks Calender.png

AUD 0.2567

Multiples of: 1000

Wirewound0805 (2012 METRIC)Unshielded100 nH5 %400 mA460 mOhms - 40 C+ 150 C651.2 GHzStandard2.3 mm1.8 mm1.6 mm CeramicAEC - Q2000805ASReel
PM0603-68NJ-RC


RF Inductors - SMD 68nH 5%
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Bourns 0
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AUD 0.2724

Multiples of: 1

 0603 (1608 METRIC)Unshielded68 nH5 %600 mA340 mOhms - 40 C+ 125 C401.7 GHzStandard1.65 mm1.05 mm1 mm Alumina PM0603Reel , Cut Tape
0805AS-R18J-08


RF Inductors - SMD Wire-wound Ceramic RF Chip Inductor
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Fastron 0
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AUD 0.2575

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded180 nH5 %400 mA640 mOhms - 40 C+ 150 C50870 MHzStandard2.3 mm1.8 mm1.6 mm CeramicAEC - Q2000805ASReel
CW252016-R10G


RF Inductors - SMD 100nH 5% HIGH Q
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Bourns 0
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AUD 0.2586

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded100 nH2 %500 mA180 mOhms - 40 C+ 125 C601 GHzStandard2.1 mm1.5 mm1.3 mm Ceramic CW252016Reel , Cut Tape
AL12A08N0JTR


RF Inductors - SMD 8nH 5% AIR CORE
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Kyocera AVX 0
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AUD 0.2586

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Toroidal Unshielded8 nH5 %4 A2.6 mOhms - 40 C+ 125 C14512.5 GHzStandard3.68 mm3.05 mm3.18 mm Air ALReel , Cut Tape
LQW2BANR10J00L


RF Inductors - SMD
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Murata 0
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AUD 0.2586

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Wirewound0805 (2015 METRIC)Unshielded100 nH5 %1.05 A350 mOhms-- 55 C+ 125 C661.2 GHzStandard2.09 mm1.53 mm1.42 mm-  LQW2BAReel , Cut Tape
B82422T1104J000


RF Inductors - SMD SMT-INDUCTOR 1210 100 UH 5%, AEC-Q200
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TDK 0
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AUD 0.2931

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded100 uH5 %60 mA11 Ohms-- 55 C+ 125 C208 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422TReel , Cut Tape
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