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
  
                         
PE-0805CD151GTT


RF Inductors - SMD SMD IND
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Pulse 1920
Ships to you
between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.2404

Multiples of: 1

Multilayer0805 (2012 METRIC)Unshielded149.4 nH2 %400 mA560 mOhms-- 40 C+ 125 C50920 MHzStandard2.29 mm1.68 mm1.58 mm-Ceramic CDReel , Cut Tape
MLF2012A4R7M


RF Inductors - SMD 4.7uH
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TDK 1915
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.078

Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded4.7 uH20 %30 mA700 mOhms-- 55 C+ 125 C4570 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
LQW2BAS27NJ00L


RF Inductors - SMD 27 NH 5%
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Murata 1915
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between Mon. 08 Dec to Thu. 11 Dec
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AUD 0.1408

Multiples of: 5

Wirewound0805 (2015 METRIC)Unshielded27 nH5 %500 mA250 mOhms-- 55 C+ 125 C552.58 GHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
AISC-1008HQ-R10J-T


RF Inductors - SMD FIXED IND 100NH 1A 160 MOHM SMD
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ABRACON 1915
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1705

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded100 nH5 %1 A160 mOhms - 40 C+ 125 C62820 MHzStandard2.6 mm2.1 mm1.7 mm Ceramic AISC - 1008HQReel , Cut Tape
LQW2UAS33NF00L


RF Inductors - SMD 33 NH 1%
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Murata 1915
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.3047

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded33 nH1 %1 A140 mOhms-- 55 C+ 125 C601.6 GHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
1210R-182J


RF Inductors - SMD 1.8uH 5%
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API Delevan 1915
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 2.4432

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded1.8 uH5 %454 mA900 mOhms-- 55 C+ 125 C3075 MHzStandard3.51 mm2.67 mm2.57 mm-  1210/RReel , Cut Tape
LCWC1008JR22GTAR


RF Inductors - SMD 220nH 1008 5%
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Kyocera AVX 1914
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.2057

Multiples of: 1

Wirewound1008 (2928 METRIC)Unshielded220 nH5 %500 mA840 mOhms - 40 C+ 125 C45700 MHzStandard2.92 mm2.79 mm2.13 mm Ceramic LCWCReel , Cut Tape
LQG18HN39NJ00D


RF Inductors - SMD 39 NH 5%
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Murata 1910
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between Mon. 08 Dec to Thu. 11 Dec
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AUD 0.0533

Multiples of: 10

Multilayer0603 (1608 METRIC)Unshielded39 nH5 %450 mA600 mOhms - 40 C+ 85 C121.5 GHzStandard1.6 mm0.8 mm0.8 mm-Air LQGReel , Cut Tape
MLF2012A3R9K


RF Inductors - SMD 0805 3.9uH 10%
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TDK 1910
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1111

Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded3.9 uH10 %30 mA650 mOhms-- 55 C+ 125 C4580 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
NLV32T-6R8J-EFD


RF Inductors - SMD 6.8uH 1.8ohms 180mA Wound Fer AEC-Q200
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TDK 1910
Ships to you
between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1614

Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded6.8 uH5 %180 mA1.8 Ohms-- 40 C+ 105 C3040 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
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