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
  
                         
L06031R8BGWTR


RF Inductors - SMD 1.8nH
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Kyocera AVX 2539
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.4948

Multiples of: 1

Thin Film0603 (1608 METRIC)Unshielded1.8 nH0.1 nH1 A70 mOhms-- 55 C+ 125 C2010 GHzStandard1.6 mm0.81 mm0.61 mm-  0603, 0805Reel , Cut Tape
CW160808-3N9K


Inductor RF Wirewound 0.0039uH 10% 250MHz 16Q-Factor Alumina 0.7A 0.08Ohm DCR 0603 T/R
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Bourns 2531
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.2182

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded3.9 nH10 %700 mA80 mOhms-- 40 C+ 125 C166 GHzStandard1.65 mm1.05 mm1 mm-Ceramic CW160808Reel , Cut Tape
MHQ0603P3N9BTD25


RF Inductors - SMD 0201 3.9nH Tol 0.1nH AEC-Q200
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TDK 2526
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.0814

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Multilayer0201 (0603 METRIC)Unshielded3.9 nH0.1 nH400 mA350 mOhms-- 55 C+ 125 C169.2 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
CW160808-R22J


Inductor RF Wirewound 0.22uH 5% 100MHz 25Q-Factor Alumina 0.2A 1.9Ohm DCR 0603 T/R
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Bourns 2525
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between Mon. 24 Nov to Fri. 28 Nov
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AUD 0.1694

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Wirewound0603 (1608 METRIC)Unshielded220 nH5 %200 mA1.9 Ohms-- 40 C+ 125 C25990 MHzStandard1.65 mm1.05 mm1 mm-Ceramic CW160808Reel , Cut Tape
MLG0603P9N1JT000


RF Inductors - SMD IND 0201 9.1nH Hi-Q SMD RF IND
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TDK 2522
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between Mon. 08 Dec to Thu. 11 Dec
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AUD 0.0025

Multiples of: 50

Multilayer0201 (0603 METRIC)Unshielded9.1 nH5 %250 mA900 mOhms-- 55 C+ 125 C145 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
LQG15HN5N1S02D


RF Inductors - SMD 5.1 NH +-.3NH
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Murata 2522
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between Mon. 08 Dec to Thu. 11 Dec
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AUD 0.0083

Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded5.1 nH0.3 nH600 mA160 mOhms - 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
MHQ0603P8N2HTD25


RF Inductors - SMD 0201 8.2nH Tol 0.1nH AEC-Q200
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TDK 2522
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.0789

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded8.2 nH3 %250 mA900 mOhms-- 55 C+ 125 C165.4 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
PE-1008CD680GTT


Inductor RF Chip Wirewound 68nH 2% 50MHz 65Q-Factor Ceramic 1A 70mOhm DCR 1008 T/R
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Pulse 2521
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between Mon. 24 Nov to Fri. 28 Nov
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AUD 0.2065

Multiples of: 1

Rf Chip1008 (2520 METRIC)Unshielded0.068 uH 1 A70 mOhms   651100 MHzStandard 2.79 mm  Ceramic  Tape And Reel
CW160808-12NJ


RF Inductors - SMD 12nH 5% HIGH Q
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Bourns 2520
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between Mon. 24 Nov to Fri. 28 Nov
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AUD 0.1694

Multiples of: 1

Wirewound Unshielded12 nH5 %700 mA130 mOhms-- 40 C+ 125 C304 GHzStandard1.65 mm1.05 mm1 mm-Ceramic  Reel , Cut Tape
AISC-1210HS-270K-T2


RF Inductors - SMD FIXED IND 27UH 250MA 4.2 OHM SMD
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ABRACON 2517
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1815

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded27 uH10 %250 mA4.2 Ohms280 mA- 40 C+ 85 C1025 MHzStandard3.2 mm3.05 mm1.3 mm Ferrite AISC - 1210HSReel , Cut Tape
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