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
  
                         
ATFC-0201HQ-2N2B-T


RF Inductors - SMD FIXED IND 2.2NH 500MA 200 MOHM
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ABRACON 5749
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0565

Multiples of: 1

Thin Film Chip Inductor0201 (0603 METRIC)Unshielded2.2 nH0.1 nH500 mA200 mOhms - 40 C+ 85 C146 GHzStandard0.6 mm0.3 mm0.23 mm Ceramic ATFC - 0201HQReel , Cut Tape
NLCV25T-4R7M-EFR


RF Inductors - SMD 4.7uH 684mohms 500mA 125C Wound Ferrite
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TDK 5744
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.132

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded4.7 uH20 %285 mA800 mOhms-- 40 C+ 105 C20-Standard2.5 mm2 mm1.9 mm-Ferrite NLCV - EFRReel , Cut Tape
B82422T1472K


RF Inductors - SMD 4.7uH 220mA 10% 3.2x2.5mm SMD
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TDK 5742
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AUD 0.2802

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Wirewound1210 (3225 METRIC)Unshielded4.7 uH10 %220 mA1.5 Ohms-- 55 C+ 125 C3050 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422TReel , Cut Tape
LQW15AN2N7B8ZD


RF Inductors - SMD 2.7 NH +/-0.1NH
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Murata 5740
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1212

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded2.7 nH0.1 nH1.5 A47 mOhms-- 55 C+ 125 C2814 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
B82498F3271J001


RF Inductors - SMD SMT-INDUCTOR 0805 270NH 5%
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TDK 5737
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3987

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Wirewound0805 (2012 METRIC)Unshielded270 nH5 %270 mA1 Ohms-- 55 C+ 125 C45900 MHzStandard2 mm1.3 mm1.4 mm-CeramicAEC - Q200B82498FReel , Cut Tape
L04021R5BHNTR


RF Inductors - SMD 1.5nH
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Kyocera AVX 5734
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3756

Multiples of: 1

Thin Film0402 (1005 METRIC)Unshielded1.5 nH0.1 nH400 mA200 mOhms-- 55 C+ 125 C2018 GHzStandard1 mm0.58 mm0.35 mm-  L0402Reel , Cut Tape
MHQ0603P9N1HT000


RF Inductors - SMD IND 0201 9.1nH S-HQ SMD RF IND
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TDK 5732
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0495

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded9.1 nH3 %250 mA900 mOhms-- 55 C+ 125 C165.5 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
LQG15WZ2N9B02D


RF Inductors - SMD Fixed IND 2.9nH 900mA INFOTMT
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Murata 5730
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1244

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Multilayer0402 (1005 METRIC)Unshielded2.9 nH0.1 nH900 mA80 mOhms-- 55 C+ 125 C236.5 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
PE-0805CLH2R2STS


RF Inductors - SMD 0805 2.2uH 950mA DCR=260mOhms RF
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Pulse 5723
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1467

Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded2.2 uH-950 mA250 mOhms600 mA- 40 C+ 125 C-50 MHzStandard2 mm1.2 mm0.9 mm-Ceramic PE - 0805CLHReel , Cut Tape
LQW18AN8N2G80D


RF Inductors - SMD 8.2 NH 2%
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Murata 5626
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.077

Multiples of: 10

Wirewound0603 (1608 METRIC)Unshielded8.2 nH2 %1.6 A52 mOhms-- 55 C+ 125 C384.75 GHzStandard1.65 mm0.99 mm0.9 mm-- LQWReel , Cut Tape
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