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
  
                         
MLF1005GR68JTD25


RF Inductors - SMD 0402 0.68uH 5% AEC-Q200
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TDK 12042
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AUD 0.1673
Multiples of: 1

Multilayer0402 (1005 METRIC)Shielded680 nH5 %45 mA550 mOhms-- 55 C+ 125 C30360 MHzStandard1 mm0.5 mm0.5 mm-FerriteAEC - Q200MLFReel , Cut Tape
B82422A3681K100


RF Inductors - SMD 680nH 145mA 10% 1210 SMD, AEC-Q200
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TDK 8303
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AUD 0.2861
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded680 nH10 %145 mA2.4 Ohms-- 55 C+ 145 C22280 MHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422AReel , Cut Tape
MLJ1608WR18JT000


RF Inductors - SMD 0.18uH 5% 0.2ohms 600mA
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TDK 3996
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AUD 0.0903
Multiples of: 10

NFC Inductor0603 (1608 METRIC)Shielded180 nH5 %650 mA200 mOhms700 mA- 55 C+ 125 C15440 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLJReel , Cut Tape
IMC0603ER47NJ01


RF Inductors - SMD 47nH 5%
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Vishay 2585
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AUD 0.1696
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Wirewound0603 (1608 METRIC)Unshielded47 nH5 %600 mA280 mOhms-- 40 C+ 125 C402 GHzStandard1.6 mm1.05 mm1.05 mm-Ceramic IMCReel , Cut Tape
B82422T1223K


RF Inductors - SMD 22uH 110mA 10% 3.2x2.5mm SMD
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TDK 2580
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AUD 0.2568
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded22 uH10 %110 mA3.5 Ohms-- 55 C+ 125 C2720 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422TReel , Cut Tape
CW252016-R18J


RF Inductors - SMD .18 UH 5%
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Bourns 2576
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AUD 0.2052
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Wirewound1008 (2520 METRIC)Unshielded180 nH5 %500 mA330 mOhms-- 40 C+ 125 C45750 MHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
LQG15HZ2N0B02D


RF Inductors - SMD 2 NH
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Murata 2566
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AUD 0.0837
Multiples of: 1

Multilayer  2 nH             Air LQGReel , Cut Tape
1210R-102J


RF Inductors - SMD 1.0uH 5%
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API Delevan 2553
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AUD 2.6654
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Wirewound1210 (3225 METRIC)Unshielded1 uH5 %515 mA700 mOhms-- 55 C+ 125 C30120 MHzStandard3.51 mm2.67 mm2.57 mm-Ferrite 1210/RReel , Cut Tape
CI160808-12NJ


RF Inductors - SMD 12nH 5% MultiLayer High Frequency
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Bourns 2550
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AUD 0.0448
Multiples of: 1

Multilayer0603 (1608 METRIC)Unshielded12 nH5 %300 mA400 mOhms-- 55 C+ 125 C101.65 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic CI160808Reel , Cut Tape
MLF1005GR39JT000


RF Inductors - SMD 1mm x 0.5mm x 0.5mm, -55 to +125 degC, 50mA, 0.39?H, 410mohm
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TDK 2517
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AUD 0.1552
Multiples of: 1

Multilayer0402 (1005 METRIC)Shielded390 nH5 %50 mA410 mOhms-- 55 C+ 125 C30600 MHzStandard1 mm0.5 mm0.5 mm-Ferrite MLFReel , Cut Tape
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