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
  
                         
LQG15HZR22H02D


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 1363
Ships to you
between Tue. 25 Nov to Mon. 01 Dec
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AUD 0.0125

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded220 nH3 %120 mA3.77 Ohms-- 55 C+ 125 C8450 MHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
L0201R82AHSTR\500


RF Inductors - SMD 0.82nH
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Kyocera AVX 1361
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1878

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Thin Film0201 (0603 METRIC)Unshielded820 pH0.05 nH400 mA200 mOhms-- 55 C+ 125 C828 GHzStandard0.6 mm0.325 mm0.225 mm-  Accu - LReel , Cut Tape
AIAC-1812-33NK-T


RF Inductors - SMD FIXED IND 33NH 3A 5.9 MOHM SMD
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ABRACON 1360
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.3905

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SMT Air Coil Inductor1812 (4532 METRIC)Unshielded33 nH10 %3 A5.9 mOhms - 40 C+ 125 C1002.5 MHzStandard4.7 mm3.5 mm3.5 mm Air AIAC - 1812Reel , Cut Tape
PM105SB-470L-RC


Inductor Power Shielded Bobbin Core 47uH 15% 100KHz 27Q-Factor Ferrite 1A 140mOhm DCR T/R
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Bourns 1360
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AUD 0.8333

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Wirewound Shielded47 uH15 %1 A140 mOhms-- 30 C+ 100 C2711 MHzStandard4.5 mm--9.9 mmFerrite PM105SBReel , Cut Tape
AS0825N0GTR


RF Inductors - SMD 25nH 2% SQUARE AIR C ORE
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Kyocera AVX 1358
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.337

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Wirewound2.134 mm x 1.829 mm x 2.972 mmUnshielded25 nH2 %4.4 A10 mOhms-- 40 C+ 125 C1302.5 GHzStandard2.972 mm2.134 mm1.829 mm-Air ASReel , Cut Tape
LQP03TG10NJ02D


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 1358
Ships to you
between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.0011

Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded10 nH5 %190 mA1.52 Ohms - 55 C+ 125 C114.5 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
ISC1812ERR10K


RF Inductors - SMD 0.1uH 10%
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Vishay 1358
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.634

Multiples of: 1

Molded1812 (4532 METRIC)Unshielded100 nH20 %552 mA230 mOhms-- 55 C+ 125 C30460 MHzStandard4.5 mm3.2 mm3.2 mm-  ISCReel , Cut Tape
1812R-105J


RF Inductors - SMD 1mH 5%
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API Delevan 1357
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AUD 2.255

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Molded1812 (4532 METRIC)Unshielded1 mH5 %55 mA60 Ohms-- 55 C+ 125 C302.5 MHzStandard4.83 mm3.4 mm3.4 mm-Ferrite 1812/RReel , Cut Tape
NLV32T-391J-EFD


RF Inductors - SMD 390uH 36ohms 35mA Wound Fer AEC-Q200
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TDK 1347
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1802

Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded390 uH5 %35 mA36 Ohms-- 40 C+ 105 C205 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
LQW18AN7N5C00D


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 989
Ships to you
between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.0446

Multiples of: 10

Wirewound0603 (1608 METRIC)Unshielded7.5 nH0.2 nH750 mA82 mOhms-- 55 C+ 125 C356 GHzStandard1.6 mm0.8 mm0.95 mm-  LQWReel , Cut Tape
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