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
  
                         
0603AS-R22J-01


RF Inductors - SMD 220nH 100 MHz 5% Tol
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Fastron 3821
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2024

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded220 nH5 %150 mA1.6 Ohms-- 40 C+ 150 C301 GHzStandard1.52 mm0.76 mm1 mm-CeramicAEC - Q2000603ASReel , Cut Tape
NLFV25T-220K-EF


RF Inductors - SMD 22uH 1.2ohms 105mA Wound Ferrite
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TDK 3818
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1504

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Wirewound2.5 mm x 2 mm x 1.8 mmShielded22 uH10 %105 mA1 Ohms-- 40 C+ 105 C--Standard2.5 mm2 mm1.8 mm-Ferrite NLFV25 - EFReel , Cut Tape
LQW18AS27NJ0ZD


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 3817
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1352

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded27 nH5 %600 mA220 mOhms-- 40 C+ 125 C402.8 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQW18ASR21J00D


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 3815
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0862

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded210 nH5 %200 mA2.06 Ohms-- 40 C+ 125 C27895 MHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LCWC0402J4N7GTAR


RF Inductors - SMD 4.7nH 5%
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Kyocera AVX 3812
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2473

Multiples of: 1

Wirewound0402 (1208 METRIC)Unshielded4.7 nH5 %640 mA130 mOhms-- 40 C+ 125 C154.7 GHzStandard1.19 mm0.66 mm0.64 mm-Ceramic LCWCReel , Cut Tape
WCLA3225V1-151-R


RF Inductors - SMD Chip IND 150uH 0.14A SMT 2 Pad
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Eaton 3812
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2724

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Wirewound1210 (3225 METRIC)Shielded150 uH10 %140 mA6.55 Ohms - 55 C+ 125 C105 MHz 3.6 mm2.8 mm2.4 mm Ferrite WCLAReel , Cut Tape
WCL3225-4R7-R


RF Inductors - SMD WCL Chip IND 3225 4.7uH 2 Pads
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Eaton 3811
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1595

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded4.7 uH5 %350 mA1.3 Ohms-- 40 C+ 85 C1260 MHzStandard3.5 mm2.9 mm2.25 mm-  WCLReel , Cut Tape
LQW18AN56NJ8ZD


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 3811
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1656

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded56 nH5 %770 mA260 mOhms-- 55 C+ 125 C382.6 GHzStandard1.65 mm0.99 mm0.9 mm- AEC - Q200LQWReel , Cut Tape
L06036R8CGSTR


RF Inductors - SMD 6.8nH CASE SIZE 0603
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Kyocera AVX 3810
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.5088

Multiples of: 1

Thin Film0603 (1608 METRIC)Unshielded6.8 nH0.2 nH300 mA300 mOhms-- 55 C+ 125 C234.5 GHzStandard1.6 mm0.81 mm0.61 mm-  0603, 0805Reel , Cut Tape
LQW15AN6N5B00D


6.5nH 90mO 0402 Inductors (SMD) ROHS
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Murata 3744
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0437

Multiples of: 10

Wirewound0402 (1005 METRIC)Unshielded6.5 nH0.1 nH700 mA90 mOhms-- 55 C+ 125 C256 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
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