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
  
                         
LQW15AN4N5B80D


RF Inductors - SMD
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Murata 2139
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AUD 0.1228
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Wirewound0402 (1005 METRIC)Unshielded4.5 nH0.1 nH1.45 A60 mOhms-- 55 C+ 125 C349.6 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
AISC-0603-R11G-T


RF Inductors - SMD FIXED IND 110NH 250MA 730 MOHM
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ABRACON 2139
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AUD 0.1907
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Wirewound0603 (1812 METRIC)Unshielded110 nH2 %250 mA730 mOhms - 40 C+ 125 C321.7 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - 0603Reel , Cut Tape
ILSB1206ERR68K


RF Inductors - SMD .68uH 10%
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Vishay 2130
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AUD 0.1231
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Established Reliability1206 (3216 METRIC)Shielded680 nH10 %150 mA800 mOhms-- 55 C+ 125 C25121 MHzStandard3.2 mm1.6 mm1.1 mm-  ILSB - 1206Reel , Cut Tape
NLV25T-820J-EF


RF Inductors - SMD 82uH 19ohms 66mA Wound Ferrite
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TDK 2127
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AUD 0.1376
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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded82 uH5 %66 mA19 Ohms-- 40 C+ 105 C2013 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
NLFV32T-6R8M-EF


RF Inductors - SMD 3.2mm x 2.5mm x 2.2mm, -40 to +105 degC, 260mA, 6.8?H, 204mohm
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TDK 2125
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AUD 0.2017
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Wirewound1210 (3225 METRIC)Shielded6.8 uH20 %260 mA170 mOhms-- 40 C+ 105 C--Standard3.2 mm2.5 mm2.2 mm-Ferrite NLFV32 - EFReel , Cut Tape
MLG0603P3N9BTD25


RF Inductors - SMD IND 0201 3.9nH Hi-Q AEC Q200 RF IND
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TDK 2122
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AUD 0.026
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Multilayer0201 (0603 METRIC)Unshielded3.9 nH0.1 nH400 mA300 mOhms - 55 C+ 125 C147.1 GHzStandard0.6 mm0.3 mm0.33 mm CeramicAEC - Q200MLG - PReel , Cut Tape
B82496C3470G000


RF Inductors - SMD SMT-INDUCTOR 0603 47NH 2%
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TDK 2121
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AUD 0.2894
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Wirewound0603 (1608 METRIC)Unshielded47 nH2 %270 mA950 mOhms-- 55 C+ 150 C142.5 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200SIMID - CReel , Cut Tape
NLV32T-1R2J-EF


RF Inductors - SMD 1.2uH 750mohms 390mA Wound Ferrite
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TDK 2104
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AUD 0.0515
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Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded1.2 uH5 %390 mA750 mOhms-- 40 C+ 105 C30100 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
MLF1608DR27JT000


RF Inductors - SMD 1.6mm x 0.8mm x 0.8mm, -55 to +125 degC, 150mA, 0.27?H, 600mohm
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TDK 2027
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AUD 0.0418
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Multilayer0603 (1608 METRIC)Shielded270 nH5 %150 mA600 mOhms-- 55 C+ 125 C15350 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
LQW15AN2N3C10D


RF Inductors - SMD
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Murata 1988
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AUD 0.0567
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Wirewound0402 (1005 METRIC)Unshielded2.3 nH0.2 nH1 A27 mOhms-- 55 C+ 125 C2514 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
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