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
  
                         
7447880068


RF Inductors - SMD WE-MK DCRes=0.25Ohms 0805 6.8nH AEC-Q200
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Wurth 4850
Ships to you
by Thu. 02 Jul
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AUD 0.1959

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Multilayer0805 (2012 METRIC)Shielded6.8 nH5 %300 mA250 mOhms - 55 C+ 125 C152.8 GHz 2 mm1.25 mm0.85 mm   WE - MKReel , Cut Tape
0805AS-068J-01


RF Inductors - SMD 68nH 200 MHz 5% Tol
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Fastron 4850
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.1895

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded68 nH5 %400 mA380 mOhms-- 40 C+ 150 C651.45 GHzStandard2.3 mm1.8 mm1.6 mm-CeramicAEC - Q2000805ASReel , Cut Tape
744901010


RF Inductors - SMD WE-TCI Thinfilm 1nH 700mA .1Ohm
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Wurth 4850
Ships to you
by Thu. 02 Jul
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AUD 0.2024

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Thin Film0402 (1005 METRIC)Shielded1 nH2 %700 mA100 mOhms-- 40 C+ 125 C1312 GHzStandard1 mm0.5 mm0.32 mm-  WE - TCIReel , Cut Tape
WCLA1608V1-271-R


RF Inductors - SMD WCLA Auto Chip IND 1608 270nH 2 Pads
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Eaton 4850
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.2181

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Wirewound0603 (1608 METRIC)Unshielded270 nH5 %170 mA2.3 Ohms-- 40 C+ 125 C24900 MHzStandard1.78 mm1.1 mm0.95 mm- AEC - Q200WCLAReel , Cut Tape
74479053


RF Inductors - SMD WE-MI SMT 0805 3.3 uH +/-10% IR = 30 mA RDC = 0.8 Ohms
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Wurth 4850
Ships to you
by Thu. 02 Jul
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AUD 0.2294

Multiples of: 1

 0805 (2012 METRIC) 3.3 uH10 %30 mA800 mOhms - 40 C+ 85 C4545 MHzStandard2 mm1.25 mm1.2 mm Ceramic WE - MIReel , Cut Tape
WCLA1005V1-120-R


RF Inductors - SMD WCLA Auto Chip IND 1005 12nH 2 Pads
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Eaton 4850
Ships to you
between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.2323

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded12 nH5 %640 mA120 mOhms-- 40 C+ 125 C253.6 GHzStandard1.19 mm0.66 mm0.6 mm- AEC - Q200WCLAReel , Cut Tape
WCLA1005V1-200-R


RF Inductors - SMD WCLA Auto Chip IND 1005 20nH 2 Pads
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Eaton 4850
Ships to you
between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.242

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded20 nH5 %420 mA250 mOhms-- 40 C+ 125 C253 GHzStandard1.19 mm0.66 mm0.6 mm- AEC - Q200WCLAReel , Cut Tape
WCLA1005V1-230-R


RF Inductors - SMD WCLA Auto Chip IND 1005 23nH 2 Pads
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Eaton 4850
Ships to you
between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.242

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded23 nH5 %310 mA380 mOhms-- 40 C+ 125 C222.72 GHzStandard1.19 mm0.66 mm0.6 mm- AEC - Q200WCLAReel , Cut Tape
HL021R1BTTR


RF Inductors - SMD 1.1nH
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Kyocera AVX 4850
Ships to you
between Wed. 08 Jul to Tue. 14 Jul
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AUD 0.2603

Multiples of: 1

Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded1.1 nH0.1 nH410 mA100 mOhms-- 55 C+ 125 C157 GHzStandard1 mm0.58 mm0.35 mm   HLReel
HL021R6BTTR


RF Inductors - SMD 1.6nH
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Kyocera AVX 4850
Ships to you
between Wed. 08 Jul to Tue. 14 Jul
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AUD 0.2685

Multiples of: 1

Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded1.6 nH0.1 nH230 mA150 mOhms-- 55 C+ 125 C157 GHzStandard1 mm0.58 mm0.35 mm   HLReel
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