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
  
                         
B82432C1333K000


RF Inductors - SMD 1812 33uH 10%
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TDK 4572
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between Thu. 23 Jul to Mon. 27 Jul
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AUD 0.5603

Multiples of: 1

Wirewound1812 (4532 METRIC)Unshielded33 uH10 %230 mA1.85 Ohms-- 55 C+ 150 C3013 MHzStandard4.5 mm3.2 mm3.2 mm-FerriteAEC - Q200B82432CReel , Cut Tape
L08052R2DESTR


RF Inductors - SMD 2.2nH 2000mA 0805 DC =0.07ohm
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Kyocera AVX 0
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AUD 0.5025

Multiples of: 3000

 0805 (2012 METRIC)Unshielded2.2 nH0.5 nH2 A70 mOhms - 55 C+ 125 C4210 GHzStandard2.11 mm1.5 mm0.91 mm   0603, 0805Reel
LQH2HNH220J03L


RF Inductors - SMD 22uH 95mA 5% PWRTRN AEC-Q200
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Murata 0
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AUD 0.5042

Multiples of: 1

Wirewound2.5 mm x 2 mm x 0.5 mmUnshielded22 uH5 % 2.75 Ohms - 40 C+ 125 C 21 MHzStandard2.5 mm2 mm0.9 mm  AEC - Q200LQH2HNH_03Reel , Cut Tape
AS0605N5GTR


RF Inductors - SMD 5.5nH 2% SQUARE AIR CORE
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AUD 0.5138

Multiples of: 1

Wirewound1.829 mm x 1.379 mm x 1.346 mmUnshielded5.5 nH2 %2.9 A3.4 mOhms-- 40 C+ 125 C604.9 GHzStandard1.346 mm1.829 mm1.397 mm-Air ASReel , Cut Tape
ISC1008ER4R7M


RF Inductors - SMD ISC-1008 4.7 20% ER e3
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Vishay 0
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AUD 0.5109

Multiples of: 1

 1008 (2520 METRIC)    15 mOhms     Standard      ISC - 1008Reel , Cut Tape
L06031R5BGWTR


RF Inductors - SMD 1.5nH
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AUD 0.523

Multiples of: 1

Thin Film0603 (1608 METRIC)Unshielded1.5 nH0.1 nH1 A60 mOhms-- 55 C+ 125 C2610 GHzStandard1.6 mm0.81 mm0.61 mm-  0603, 0805Reel
0402DC-6N2XGRW


RF Inductors - SMD 1005 6.2nH Unshld 2% 1.8A 57mOhms
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Coilcraft 0
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AUD 0.5303

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded6.2 nH2 %1.8 A57 mOhms-- 40 C+ 125 C1469.2 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
AISC-1206-R56J-T


RF Inductors - SMD FIXED IND 560NH 460MA 1.34 OHM
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ABRACON 0
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AUD 0.5327

Multiples of: 1

Ceramic Wirewound RF Inductor1206 (3216 METRIC)Unshielded560 nH5 %460 mA1.34 Ohms - 40 C+ 125 C45470 MHzStandard3.56 mm2.16 mm1.52 mm Ceramic AISC - 1206Reel , Cut Tape
5508 151 34 00


RF Inductors - SMD RF Chip Inductor SMD 150nH 0805 5% Tol
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Sumida 0
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AUD 0.5348

Multiples of: 1

 0805 (2012 METRIC)Unshielded150 nH5 %270 mA440 mOhms - 55 C+ 125 C351.12 GHzStandard2.2 mm1.4 mm1.42 mm   5508Reel
L0603100GGSTR\500


RF Inductors - SMD 10nH 300mA 2% 0603 S MD High Q RF
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AUD 0.5697

Multiples of: 1

 0603 (1608 METRIC)Unshielded10 nH2 %300 mA450 mOhms - 55 C+ 125 C283.5 GHzStandard1.6 mm0.81 mm0.61 mm   0603, 0805Reel , Cut Tape
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