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
  
                         
LQG18HH3N3S00D


RF Inductors - SMD 3.3 NH +-.3 NH
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Murata 4113
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1339

Multiples of: 1

Multilayer0603 (1608 METRIC)Unshielded3.3 nH0.3 nH900 mA140 mOhms-- 55 C+ 125 C124 GHzStandard1.6 mm0.8 mm0.8 mm-AirAEC - Q200LQGReel , Cut Tape
MHQ0603P4N0BT000


RF Inductors - SMD IND 0201 4.0nH S-HQ SMD RF IND
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TDK 4102
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0727

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded4 nH0.1 nH400 mA350 mOhms-- 55 C+ 125 C168.5 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
B82432C1223K


RF Inductors - SMD SMT-INDUCTOR 1812 22 UH 10%, AEC-Q200
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TDK 4101
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.6078

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Wirewound1812 (4532 METRIC)Unshielded22 uH10 %260 mA1.45 Ohms-- 55 C+ 150 C3016 MHzStandard4.5 mm3.2 mm3.2 mm-FerriteAEC - Q200B82432CReel , Cut Tape
LQG15WH15NJ02D


RF Inductors - SMD 15 NH 5% NH
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Murata 4094
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.07

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded15 nH5 %400 mA280 mOhms-- 55 C+ 125 C232.3 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
NLV32T-101J-EF


RF Inductors - SMD 100uH 10ohms 40mA Wound Ferrite
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TDK 4093
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0506

Multiples of: 10

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded100 uH5 %40 mA10 Ohms-- 40 C+ 105 C2010 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
0805AS-R10J-01


RF Inductors - SMD 100nH 150 MHz 5% Tol
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Fastron 4089
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.187

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded100 nH5 %400 mA460 mOhms-- 40 C+ 150 C651.2 GHzStandard2.3 mm1.8 mm1.6 mm-CeramicAEC - Q2000805ASReel , Cut Tape
CW201212-8N2J


RF Inductors - SMD 8.2nH 5%
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Bourns 4086
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2007

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded8.2 nH5 %600 mA60 mOhms-- 40 C+ 125 C605.5 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW201212Reel , Cut Tape
LQP03TQ1N2B02D


RF Inductors - SMD 1.2nH 800mA 0201 (0603 metric) SUGGESTED ALT LQP03HQ1N2B02D
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Murata 4075
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.033

Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded1.2 nH0.1 nH800 mA80 mOhms-- 55 C+ 125 C1717 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
HL022R4BTTR


RF Inductors - SMD 2.4nH
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Kyocera AVX 4074
Ships to you
between Fri. 21 Nov to Thu. 27 Nov
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AUD 0.2916

Multiples of: 1

Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded2.4 nH0.1 nH230 mA200 mOhms-- 55 C+ 125 C157 GHzStandard1 mm0.58 mm0.35 mm-  HLReel , Cut Tape
LQP03TG27NH02D


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 3492
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0063

Multiples of: 50

Thin Film0201 (0603 METRIC)Unshielded27 nH3 %120 mA3.65 Ohms-- 55 C+ 125 C71.7 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
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