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
  
                         
AL023538NJTS


RF Inductors - SMD 538nH 5% AIR CORE
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Kyocera AVX 1649
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.2846

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Toroidal Unshielded538 nH5 %2 A90 mOhms - 40 C+ 125 C87490 MHzStandard10.55 mm6.35 mm5.9 mm Air ALReel , Cut Tape
4426R-7


RF Inductors - SMD 22.0 uH 5%
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API Delevan 1649
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AUD 2.2212

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Wirewound1812 (4532 METRIC)Unshielded22 nH5 %3 A450 mOhms-- 55 C+ 125 C1023 GHzStandard6.86 mm3.05 mm3.18 mm-Air 4426/RReel , Cut Tape
MHQ1005P3N3ST000


RF Inductors - SMD IND 0402 3.3nH S-HQ SMD RF IND
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TDK 1647
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.105

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Multilayer0402 (1005 METRIC)Unshielded3.3 nH0.3 nH900 mA80 mOhms-- 55 C+ 125 C239 GHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
ILSB0805ERR56K


RF Inductors - SMD .56uH 10%
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Vishay 1647
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1174

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Established Reliability0805 (2012 METRIC)Shielded560 nH10 %150 mA750 mOhms-- 55 C+ 125 C25133 MHzStandard2 mm1.25 mm0.9 mm-  ILSB - 0805Reel , Cut Tape
MLF2012E8R2K


RF Inductors - SMD 0805 8.2uH 10%
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TDK 1641
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.0953

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Multilayer0805 (2012 METRIC)Shielded8.2 uH10 %15 mA700 mOhms-- 55 C+ 125 C5055 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
NLFV32T-3R3M-EFT


RF Inductors - SMD 3.3uH 0.11ohms 420mA +/-20%
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TDK 1640
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.2868

Multiples of: 1

Wirewound1210 (3225 METRIC)Shielded3.3 uH20 %420 mA110 mOhms-- 40 C+ 105 C--Standard3.2 mm2.5 mm2.2 mm-Ferrite NLFV - EFTReel , Cut Tape
LQW18CNR16J00D


RF Inductors - SMD 160 NH 5%
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Murata 1639
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between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.1211

Multiples of: 5

Wirewound0603 (1608 METRIC)Unshielded160 nH5 %1 A100 mOhms-- 40 C+ 85 C-900 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite LQWReel , Cut Tape
AISC-0805-R039G-T


RF Inductors - SMD FIXED IND 39NH 500MA 290 MOHM
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Abracon 1638
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.2988

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Wirewound0805 (2317 METRIC)Unshielded39 nH2 %500 mA290 mOhms - 40 C+ 125 C602 GHzStandard2.29 mm1.73 mm1.55 mm Ceramic AISC - 0805Reel , Cut Tape
1008AS-047J-01


RF Inductors - SMD 47nH 50 MHz 5% Tol
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Fastron 1634
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1955

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded47 nH5 %1 A160 mOhms-- 40 C+ 125 C651.5 GHzStandard2.9 mm2.8 mm2.1 mm-CeramicAEC - Q2001008ASReel , Cut Tape
PM0805-2N2M-RC


RF Inductors - SMD 2.2nH 20%
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Bourns 1629
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.2868

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded2.2 nH20 %600 mA8 mOhms-- 55 C+ 125 C15 Standard2.1 mm1.5 mm1.3 mm-Ceramic PM0805Reel , Cut Tape
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