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
  
                         
AISC-1210HS-5R6K-T2


RF Inductors - SMD FIXED IND 5.6UH 520MA 1 OHM SMD
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ABRACON 1940
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.2159

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded5.6 uH10 %520 mA1 Ohms550 mA- 40 C+ 85 C1065 MHzStandard3.2 mm3.05 mm1.3 mm Ferrite AISC - 1210HSReel , Cut Tape
0603AS-010J-08


RF Inductors - SMD 10nH 250 MHz 5%
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Fastron 1940
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between Mon. 24 Nov to Fri. 28 Nov
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AUD 0.2263

Multiples of: 1000

Wirewound0603 (1608 METRIC)Unshielded10 nH5 %700 mA130 mOhms-- 40 C+ 150 C314.8 GHzStandard1.52 mm0.76 mm1 mm-CeramicAEC - Q2000603ASReel , Cut Tape
0603AS-R10J-08


RF Inductors - SMD 100nH 150 MHz 5% Tol
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Fastron 1940
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between Mon. 24 Nov to Fri. 28 Nov
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AUD 0.2263

Multiples of: 1000

Wirewound0603 (1608 METRIC)Unshielded100 nH5 %400 mA580 mOhms - 40 C+ 150 C341.4 GHzStandard1.7 mm1.1 mm1 mm CeramicAEC - Q2000603ASReel , Cut Tape
PE-0603CD270JTT


RF Inductors - SMD SMD IND
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Pulse 1940
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between Mon. 24 Nov to Fri. 28 Nov
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AUD 0.2277

Multiples of: 1

Multilayer0603 (1608 METRIC)Unshielded27 nH5 %600 mA220 mOhms - 40 C+ 125 C352.8 GHzStandard1.8 mm1.24 mm1.02 mm-Ceramic CDReel , Cut Tape
PE-1206CD100JTT


RF Inductors - SMD 1206 SMD IND CERAMIC
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Pulse 1940
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between Mon. 24 Nov to Fri. 28 Nov
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AUD 0.2357

Multiples of: 1

Multilayer1206 (3216 METRIC)Unshielded10 nH5 %1 A80 mOhms-- 40 C+ 125 C404 GHzStandard3.56 mm2.16 mm1.52 mm-Ceramic CDReel , Cut Tape
PM0805-R39K-RC


RF Inductors - SMD 0.39uH 10%
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Bourns 1940
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.25

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded390 nH10 %200 mA1.5 Ohms-- 55 C+ 125 C45420 MHzStandard2.1 mm1.5 mm1.3 mm-Ceramic PM0805Reel , Cut Tape
PE-0603CD470GTT


RF Inductors - SMD SMD IND
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Pulse 1940
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between Mon. 24 Nov to Fri. 28 Nov
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AUD 0.2589

Multiples of: 2000

Multilayer0603 (1608 METRIC)Unshielded47 nH2 %600 mA280 mOhms-- 40 C+ 125 C352 GHzStandard1.8 mm1.24 mm1.02 mm-Ceramic CDReel , Cut Tape
36502AR56JTDG


RF Inductors - SMD 3650 2A 0.56uH 5% 2K RL
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TE Connectivity 1940
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AUD 0.291

Multiples of: 2000

Wirewound0805 (2012 METRIC)Unshielded560 nH5 %210 mA1.9 Ohms-- 40 C+ 125 C23340 MHzStandard2.29 mm1.73 mm1.52 mm-  3650Reel , Cut Tape
LQW2UASR75F00L


RF Inductors - SMD
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Murata 1940
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.3006

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded750 nH1 %360 mA1.54 Ohms-- 55 C+ 125 C45360 MHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
6-1624113-1


3650 0805 0.47uH 5% 2K R
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TE Connectivity 1940
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between Mon. 24 Nov to Fri. 28 Nov
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AUD 0.3008

Multiples of: 2000

                     
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