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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(Ex. GST)(▲▼)		Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
MLF1005VR33JTD25


RF Inductors - SMD 0402 0.33uH 5% AEC-Q200
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TDK 1526
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AUD 0.1502
Multiples of: 1

Multilayer0402 (1005 METRIC)Shielded330 nH5 %140 mA1.05 Ohms-- 55 C+ 125 C15380 MHzStandard1 mm0.5 mm0.5 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQW18AN22NJ0ZD


RF Inductors - SMD
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Murata 1524
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AUD 0.1035
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded22 nH5 %500 mA17 mOhms-- 55 C+ 125 C404.6 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
NLV32T-R12J-EF


RF Inductors - SMD 120nH 220mohms 450mA Wound Ferrite
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TDK 1518
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AUD 0.0522
Multiples of: 5

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded120 nH5 %450 mA220 mOhms-- 40 C+ 105 C30500 MHzStandard3.2 mm2.5 mm2.2 mm Ferrite NLV32 - EFReel , Cut Tape
CW252016-22NK


Inductor RF Wirewound 0.022uH 10% 50MHz 55Q-Factor Ceramic 1A 0.12Ohm DCR 1008 T/R
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Bourns 1514
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AUD 0.2166
Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded22 nH10 %600 mA100 mOhms-- 40 C+ 125 C602.4 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
B82422A1153K100


RF Inductors - SMD 15uH 165mA 10% 1210 SMD, AEC-Q200
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TDK 1504
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AUD 0.3025
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded15 uH10 %165 mA1.85 Ohms-- 55 C+ 145 C2720 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
MLF2012DR15JT000


RF Inductors - SMD 2mm x 1.25mm x 0.85mm, -55 to +125 degC, 300mA, 0.15?H, 200mohm
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TDK 1503
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AUD 0.0563
Multiples of: 10

Multilayer0805 (2012 METRIC)Shielded150 nH5 %300 mA200 mOhms-- 55 C+ 125 C20410 MHzStandard2 mm1.25 mm0.85 mm-Ferrite MLFReel , Cut Tape
L08055R6DEWTR


RF Inductors - SMD 5.6nH
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Kyocera AVX 1487
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AUD 0.9936
Multiples of: 1

Thin Film0805 (2012 METRIC)Unshielded5.6 nH0.5 nH1.5 A100 mOhms-- 55 C+ 125 C504.6 GHzStandard2.11 mm1.5 mm0.91 mm-  0603, 0805Reel , Cut Tape
IMC0805ER2R7J01


RF Inductors - SMD 2.7uH 5%
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Vishay 1486
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AUD 0.2201
Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded2.7 nH0.3 nH800 mA80 mOhms-- 40 C+ 125 C356 GHzStandard2 mm1.25 mm1.2 mm-Ceramic IMCReel , Cut Tape
L0805120JEWTR


RF Inductors - SMD 12nH 5%
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Kyocera AVX 1486
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AUD 0.9955
Multiples of: 1

Thin Film0805 (2012 METRIC)Unshielded12 nH5 %1.5 A200 mOhms-- 55 C+ 125 C402.4 GHzStandard2.11 mm1.5 mm0.91 mm-  0603, 0805Reel , Cut Tape
LQG15HN33NH02D


RF Inductors - SMD
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Murata 1435
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AUD 0.0345
Multiples of: 20

Multilayer0402 (1005 METRIC)Unshielded33 nH3 %300 mA670 mOhms-- 55 C+ 125 C81.5 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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