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
  
                         
LQP02TN2N1B02D


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 15583
Ships to you
between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.0485

Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded2.1 nH0.1 nH200 mA750 mOhms - 55 C+ 125 C89 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
LQW15AN11NH00D


RF Inductors - SMD
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Murata 15533
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between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.0785

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded11 nH3 %500 mA140 mOhms-- 55 C+ 125 C305.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
NLV25T-270J-EF


RF Inductors - SMD 27uH 6.3ohms 115mA Wound Ferrite
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TDK 15523
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between Fri. 13 Feb to Thu. 19 Feb
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AUD 0.0412

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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded27 uH5 %115 mA6.3 Ohms-- 40 C+ 105 C2521 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
LCCI0603S2N2GTAR


RF Inductors - SMD 2.2nH Tol 0.3nH 0603 1000mA DCR=0.1 Ohms
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Kyocera AVX 15520
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between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.0302

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Multilayer0603 (1608 METRIC)Unshielded2.2 nH0.3 nH1 A100 mOhms-- 40 C+ 85 C88 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic LCCIReel , Cut Tape
CS160808-R68K


RF Inductors - SMD 0.68uH '10%
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Bourns 15520
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between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.077

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Multilayer0603 (1608 METRIC)Shielded680 nH10 %150 mA900 mOhms-- 55 C+ 125 C3080 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite  Reel , Cut Tape
MHQ1005075HA2N2BTD25


RF Inductors - SMD FIXED IND 2.2NH 1A 50 MOHM SMD
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TDK 15520
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between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.1187

Multiples of: 1

Multilayer Ceramic Inductor0402 (1005 METRIC)Shielded2.2 nH0.1 nH1 A50 mOhms - 55 C+ 125 C2013.1 GHzStandard1 mm0.5 mm0.7 mm Ceramic MHQReel , Cut Tape
LQG15WZ36NJ02D


RF Inductors - SMD Fixed IND 36nH 190mA INFOTMT
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Murata 15447
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between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.0632

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Multilayer0402 (1005 METRIC)Unshielded36 nH5 %190 mA1.5 Ohms-- 55 C+ 125 C201.6 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQW15AN1N5D8ZD


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 15387
Ships to you
between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.1212

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded1.5 nH0.5 nH2.1 A28 mOhms-- 55 C+ 125 C2018 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LQW18ASR12G00D


RF Inductors - SMD
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Murata 15381
Ships to you
between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.0879

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded120 nH2 %300 mA650 mOhms-- 40 C+ 125 C321.3 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LCCI0603J6N8GTAR


RF Inductors - SMD 6.8nH Tol 5% 0603 60 0mA DCR=0.25 Ohms
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Kyocera AVX 15364
Ships to you
between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.0424

Multiples of: 1

Multilayer0603 (1608 METRIC)Unshielded6.8 nH5 %600 mA250 mOhms-- 40 C+ 85 C104 GHzStandard1.6 mm0.8 mm0.8 mm-  LCCIReel , Cut Tape
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