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
  
                         
MLF1608DR22JTD25


RF Inductors - SMD 220nH 550mohms 150mA +/-5% Fer AEC-Q200
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TDK 5579
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AUD 0.1483
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Multilayer0603 (1608 METRIC)Shielded220 nH5 %150 mA550 mOhms-- 55 C+ 125 C15400 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
L06031R2CGSTR


RF Inductors - SMD 1.2nH
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Kyocera AVX 5578
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AUD 0.4164
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Thin Film0603 (1608 METRIC)Unshielded1.2 nH0.2 nH1 A40 mOhms-- 55 C+ 125 C4910 GHzStandard1.6 mm0.81 mm0.61 mm-  0603, 0805Reel , Cut Tape
CI160808-56NJ


RF Inductors - SMD 56nH 5% MultiLayer High Frequency
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Bourns 5572
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AUD 0.0423
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Multilayer0603 (1608 METRIC)Unshielded56 nH5 %300 mA1 Ohms-- 55 C+ 125 C101.15 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic CI160808Reel , Cut Tape
B82422A3680K100


RF Inductors - SMD 68nH 480mA 10% 1210 SMD, AEC-Q200
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TDK 5566
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AUD 0.3736
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Wirewound1210 (3225 METRIC)Unshielded68 nH10 %480 mA210 mOhms-- 55 C+ 145 C271.15 GHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422AReel , Cut Tape
LQW15AN12NJ8ZD


RF Inductors - SMD
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Murata 5559
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AUD 0.1232
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Wirewound0402 (1005 METRIC)Unshielded12 nH5 %1.24 A93 mOhms-- 55 C+ 125 C305.2 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
B82498F3181J001


RF Inductors - SMD SMT-INDUCTOR 0805 180NH 5%
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TDK 5549
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AUD 0.4604
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Wirewound0805 (2012 METRIC)Unshielded180 nH5 %340 mA530 mOhms-- 55 C+ 125 C451.05 GHzStandard2 mm1.3 mm1.4 mm-CeramicAEC - Q200B82498FReel , Cut Tape
KLZ2012MHR4R7WTD25


RF Inductors - SMD 4.7uH 2MHz 20% 2012 AEC-Q200
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TDK 5542
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AUD 0.1452
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Multilayer0805 (2012 METRIC)Shielded4.7 uH20 %170 mA500 mOhms180 mA- 55 C+ 150 C--Flexible (Soft)2 mm1.25 mm0.85 mm-FerriteAEC - Q200KLZ - HRReel , Cut Tape
B82498F3821J


RF Inductors - SMD 820nH 180mA 5% 2.3x1.7mm SMD
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TDK 5514
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AUD 0.3534
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Wirewound0805 (2012 METRIC)Unshielded820 nH5 %180 mA1.9 Ohms-- 55 C+ 125 C23300 MHzStandard2 mm1.3 mm1.4 mm-Ceramic B82498FReel , Cut Tape
MLF1608A2R2JT000


RF Inductors - SMD 1.6mm x 0.8mm x 0.8mm, -55 to +125 degC, 30mA, 2.2?H, 1ohm
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TDK 4850
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AUD 0.0429
Multiples of: 20

Multilayer0603 (1608 METRIC)Shielded2.2 uH5 %30 mA1 Ohms-- 55 C+ 125 C35120 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
NLCV32T-R68M-EFR


RF Inductors - SMD 680nH 54mohms 1.9A 125C Wound Ferrite
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TDK 3402
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AUD 0.1413
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Wirewound1210 (3225 METRIC)Unshielded680 nH20 %1.9 A45 mOhms-- 40 C+ 125 C10-Standard3.2 mm2.5 mm2.2 mm-Ferrite NLCV - EFRReel , Cut Tape
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