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
  
                         
LQP02TQ0N9B02D


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 14685
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between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.0874

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Thin Film01005 (0402 METRIC)Unshielded900 pH0.1 nH580 mA150 mOhms-- 55 C+ 125 C1016.6 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
PE-0402CL1N2STT


RF Inductors - SMD 0402 1.2nH 400mA DCR=100mOhms RF
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Pulse 14674
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between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.0293

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Multilayer0402 (1005 METRIC)Unshielded1.2 nH0.3 nH400 mA100 mOhms-- 55 C+ 125 C810 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
LQW15AN16NG80D


RF Inductors - SMD 16 NH 2%
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Murata 14654
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between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.1155

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Wirewound0402 (1005 METRIC)Unshielded16 nH2 %1 A126 mOhms-- 55 C+ 125 C315 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQG15WH68NG02D


RF Inductors - SMD Fixed IND 68nH 160mA POWRTRN
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Murata 14652
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between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.1449

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Multilayer0402 (1005 METRIC)Unshielded68 nH2 %160 mA2 Ohms-- 55 C+ 125 C221.1 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
MHQ0603P3N4BTD25


RF Inductors - SMD 0201 3.4nH Tol 0.1nH AEC-Q200
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TDK 14647
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between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.1192

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Multilayer0201 (0603 METRIC)Unshielded3.4 nH0.1 nH500 mA250 mOhms-- 55 C+ 125 C169.3 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
MHQ0603P6N8HTD25


RF Inductors - SMD 0201 6.8nH Tol 0.1nH AEC-Q200
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TDK 14637
Ships to you
between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.0776

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded6.8 nH3 %300 mA700 mOhms-- 55 C+ 125 C166.8 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
MHQ1005P2N7CT000


RF Inductors - SMD IND 0402 2.7nH S-HQ SMD RF IND
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TDK 14631
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AUD 0.0965

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Multilayer0402 (1005 METRIC)Unshielded2.7 nH0.2 nH900 mA70 mOhms-- 55 C+ 125 C239.6 GHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
LQW18AN18NG8ZD


RF Inductors - SMD 18 NH 2%
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Murata 14617
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between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.1553

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Wirewound0603 (1608 METRIC)Unshielded18 nH2 %1.4 A75 mOhms - 55 C+ 125 C404.6 GHzStandard1.65 mm0.99 mm0.9 mm--AEC - Q200LQWReel , Cut Tape
MHQ0603P3N5BTD25


RF Inductors - SMD 0201 3.5nH Tol 0.1nH AEC-Q200
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TDK 14588
Ships to you
between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.0852

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Multilayer0201 (0603 METRIC)Unshielded3.5 nH0.1 nH500 mA250 mOhms-- 55 C+ 125 C169.5 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
LQP03HQ9N1J02D


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 14581
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between Thu. 19 Feb to Mon. 23 Feb
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AUD 0.0827

Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded9.1 nH5 %300 mA400 mOhms-- 55 C+ 125 C204.5 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
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