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
  
                         
MHQ0402PSA0N4CT000


RF Inductors - SMD 01005, 0.4nH +-0.2nH S-HQ SMD RF IND
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TDK 19339
Ships to you
between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.0525

Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded400 pH0.2 nH600 mA150 mOhms-- 55 C+ 125 C-20 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
MCLA1005V2-120-R


RF Inductors - SMD 12 NH 5% AEC-Q200
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Eaton 19321
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.0385

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded12 nH5 %300 mA500 mOhms-- 40 C+ 125 C82.7 GHzStandard1 mm0.5 mm0.5 mm- AEC - Q200MCLAReel , Cut Tape
MHQ0402PSA0N9ST000


RF Inductors - SMD 01005, 0.9nH +-0.3nH S-HQ SMD RF IND
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TDK 19312
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.0525

Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded900 pH0.3 nH600 mA150 mOhms-- 55 C+ 125 C-20 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQG15WH2N7B02D


RF Inductors - SMD
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Murata 19312
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.1449

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded2.7 nH0.1 nH900 mA70 mOhms-- 55 C+ 125 C236.5 GHzStandard1 mm0.6 mm0.5 mm-Air LQGReel , Cut Tape
LQW15AN51NG8ZD


RF Inductors - SMD
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Murata 19310
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.1155

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded51 nH2 %415 mA696 mOhms-- 55 C+ 125 C2.92.9 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
ILC0402ERR10J


RF Inductors - SMD ILC-0402 .1 5% ER E3
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Vishay 19305
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.0297

Multiples of: 1

                   ILC - 0402Reel , Cut Tape
MLF1005VR56JTD25


RF Inductors - SMD 0402 0.56uH 5% AEC-Q200
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TDK 19303
Ships to you
between Fri. 14 Nov to Thu. 20 Nov
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AUD 0.0078

Multiples of: 1

Multilayer0402 (1005 METRIC)Shielded560 nH5 %120 mA1.95 Ohms-- 55 C+ 125 C15250 MHzStandard1 mm0.5 mm0.5 mm-FerriteAEC - Q200MLFReel , Cut Tape
BSCH001005051N8SCP


RF Inductors - SMD 1.8nH RDC=0.10Ohms 400mA
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Pulse 19303
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between Thu. 20 Nov to Mon. 24 Nov
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AUD 0.0152

Multiples of: 1

 1 mm x 0.5 mm x 0.5 mmShielded1.8 nH0.3 nH 100 mOhms400 mA- 55 C+ 125 C88.7 GHzStandard1 mm0.5 mm0.5 mm Ceramic BSCHReel , Cut Tape
LQG15HZR27J02D


RF Inductors - SMD
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Murata 19303
Ships to you
between Fri. 14 Nov to Thu. 20 Nov
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AUD 0.0345

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded270 nH5 %110 mA4.94 Ohms-- 55 C+ 125 C8400 MHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQW15AN2N5B00D


RF Inductors - SMD 2.5 NH +-.1NH
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Murata 17101
Ships to you
between Fri. 28 Nov to Wed. 03 Dec
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AUD 0.0677

Multiples of: 10

Wirewound0402 (1005 METRIC)Unshielded2.5 nH0.1 nH850 mA50 mOhms-- 55 C+ 125 C2015 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
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