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
  
                         
NLV32T-R68J-EFD


RF Inductors - SMD 680nH 600mohms 450mA Wound Fer AEC-Q200
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TDK 1401
Ships to you
between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.1483

Multiples of: 5

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded680 nH5 %450 mA600 mOhms-- 40 C+ 105 C30160 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
AISC-1008F-3R3G-T


RF Inductors - SMD FIXED IND 3.3UH 450MA 1.7 OHM
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ABRACON 1345
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1961

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded3.3 uH2 %450 mA1.7 Ohms - 40 C+ 125 C23100 MHzStandard2.92 mm2.79 mm2.29 mm Ferrite AISC - 1008FReel , Cut Tape
LQW18ASR11G0ZD


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 1344
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1293

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded110 nH2 %300 mA610 mOhms-- 40 C+ 125 C321.35 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
AISC-1008HQ-47NJ-T


RF Inductors - SMD FIXED IND 47NH 1.2A 120 MOHM SMD
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ABRACON 1341
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.2878

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded47 nH5 %1.2 A120 mOhms - 40 C+ 125 C751.45 GHzStandard2.6 mm2.1 mm1.7 mm Ceramic AISC - 1008HQReel , Cut Tape
LQW18CNR16J0ZD


RF Inductors - SMD Fixed IND 160nH 1000mA INFOTMT
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Murata 1338
Ships to you
between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.1305

Multiples of: 5

Wirewound0603 (1608 METRIC)Unshielded160 nH5 %1 A100 mOhms-- 55 C+ 125 C-900 MHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
CW252016-R39J


390 nH Unshielded Drum Core, Wirewound Inductor 400 mA 1.12Ohm Max 1008 (2520 Metric)
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Bourns 1337
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.2

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded390 nH5 %400 mA1.2 Ohms-- 40 C+ 125 C45500 MHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
CMH322522-R15ML


RF Inductors - SMD MAGNETICS - CHIP INDUCTOR
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Bourns 1337
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.3486

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Wirewound1210 (3225 METRIC)Shielded150 nH20 %450 mA250 mOhms-- 55 C+ 125 C30450 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite CMH322522Reel , Cut Tape
AISC-0805F-2R2G-T


RF Inductors - SMD FIXED IND 2.2UH 100MA 2.5 OHM
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ABRACON 1336
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1907

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded2.2 uH2 %100 mA2.5 Ohms - 40 C+ 125 C10200 MHzStandard2.29 mm1.73 mm1.55 mm Ferrite AISC - 0805FReel , Cut Tape
1210R-392J


RF Inductors - SMD 3.9uH 5%
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API Delevan 1332
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AUD 2.6048

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Wirewound1210 (3225 METRIC)Unshielded3.9 uH5 %378 mA1.3 Ohms-- 55 C+ 125 C3050 MHzStandard3.51 mm2.67 mm2.57 mm-Ferrite 1210/RReel , Cut Tape
HL028R2BTTR


RF Inductors - SMD 8.2nH
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Kyocera AVX 1330
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between Tue. 25 Nov to Mon. 01 Dec
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AUD 0.343

Multiples of: 1

Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded8.2 nH0.1 nH115 mA800 mOhms-- 55 C+ 125 C156 GHzStandard1 mm0.58 mm0.35 mm-  HLReel , Cut Tape
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