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
  
                         
LQW15AN4N5B8ZD


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 4522
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1173

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded4.5 nH0.1 nH1.45 A60 mOhms-- 55 C+ 125 C349.6 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
B82496C3101G000


RF Inductors - SMD SMT-INDUCTOR 0603 100NH 2%
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TDK 4520
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AUD 0.2819

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Wirewound0603 (1608 METRIC)Unshielded100 nH2 %200 mA1.8 Ohms-- 55 C+ 150 C141.8 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200SIMID - CReel , Cut Tape
B82498F3470J


RF Inductors - SMD 47 nH 600mA 5% 2.3x1.7mm SMD
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TDK 4517
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.374

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Wirewound0805 (2012 METRIC)Unshielded47 nH5 %600 mA130 mOhms-- 55 C+ 125 C652 GHzStandard2 mm1.3 mm1.4 mm-Ceramic B82498FReel , Cut Tape
LQW2BAS36NJ00L


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 4512
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.124

Multiples of: 1

Wirewound0805 (2015 METRIC)Unshielded36 nH5 %500 mA270 mOhms-- 55 C+ 125 C551.9 GHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
AISC-0603-R082J-T


RF Inductors - SMD FIXED IND 82NH 300MA 500 MOHM
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ABRACON 4509
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1577

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Wirewound0603 (1812 METRIC)Unshielded82 nH5 %300 mA500 mOhms - 40 C+ 125 C342 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - 0603Reel , Cut Tape
MLJ1608WR33KT000


RF Inductors - SMD 330nH 0.24ohms 650mA 10% 230MHz
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TDK 4507
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1504

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NFC Inductor0603 (1608 METRIC)Shielded330 nH10 %500 mA320 mOhms650 mA- 55 C+ 125 C15320 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLJReel , Cut Tape
WCLA2520V1-R22-R


RF Inductors - SMD Chip IND 0.22uH 1.1A SMT 2 Pad
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Eaton 4505
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2287

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Wirewound1008 (2520 METRIC)Shielded220 nH10 %1.1 A500 mOhms - 55 C+ 125 C30450 MHz 2.9 mm2.5 mm2.1 mm Ferrite WCLAReel , Cut Tape
MLF1608D47NMTA00


200mA 47nH ±20% 100mO 0603 Inductors (SMD) ROHS
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TDK 4495
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0459

Multiples of: 5

Multilayer0603 (1608 METRIC)Shielded47 nH20 %200 mA200 mOhms-- 55 C+ 125 C10900 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
LQP03HQ2N5B02D


RF Inductors - SMD 2.5 NH +/-0.1NH
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Murata 4442
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0335

Multiples of: 20

Thin Film0201 (0603 METRIC)Unshielded2.5 nH0.1 nH600 mA120 mOhms-- 55 C+ 125 C209 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
MLG0603P2N7BT000


RF Inductors - SMD IND 0201 2.7nH Hi-Q SMD RF IND
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TDK 4025
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.005

Multiples of: 50

Multilayer0201 (0603 METRIC)Unshielded2.7 nH0.1 nH500 mA200 mOhms-- 55 C+ 125 C1410 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
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