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
  
                         
LQP03TNR24J02D


Inductor RF Chip Thin Film 240nH 5% 100MHz 5Q-Factor 60mA 15Ohm DCR 0201 T/R
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Murata 10078
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AUD 0.033
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded240 nH5 %60 mA15 Ohms - 55 C+ 125 C5450 MHzStandard0.6 mm0.3 mm0.3 mm Ferrite LQPReel , Cut Tape
MLG1005S3N9BTD25


RF Inductors - SMD IND 0402 3.9nH StdQ AEC Q200 RF IND
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TDK 10068
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AUD 0.0182
Multiples of: 20

Multilayer0402 (1005 METRIC)Unshielded3.9 nH0.1 nH700 mA200 mOhms-- 55 C+ 125 C86.5 GHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
CIGT252008LM1R0MNE


RF Inductors - SMD CIGT,Thin Film,1008,1.0uH,0.8?,7 embossed,-20 20%
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SAMSUNG 10045
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AUD 0.139
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Thin Film  1 uH20 %              CIGTReel , Cut Tape
LQG15HS15NH02D


RF Inductors - SMD 15 NH 3%
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Murata 10039
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AUD 0.018
Multiples of: 50

Multilayer0402 (1005 METRIC)Unshielded15 nH3 %450 mA320 mOhms-- 55 C+ 125 C82.5 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQW15AN39NG00D


RF Inductors - SMD 39 NH 2%
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Murata 10029
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AUD 0.0362
Multiples of: 20

Wirewound0402 (1005 METRIC)Unshielded39 nH2 %250 mA700 mOhms-- 55 C+ 125 C253 GHzStandard1 mm0.5 mm0.5 mm-  LQWReel , Cut Tape
B82496C3680J


RF Inductors - SMD 68nH 230mA 5% 1.6x0.8mm SMD
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TDK 10027
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AUD 0.181
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Wirewound0603 (1608 METRIC)Unshielded68 nH5 %230 mA1.3 Ohms-- 55 C+ 150 C142 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200SIMID - CReel , Cut Tape
LQW15AN1N5C8ZD


RF Inductors - SMD
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Murata 10024
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AUD 0.1131
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded1.5 nH0.2 nH2.1 A28 mOhms-- 55 C+ 125 C2018 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQW15AN47NG8ZD


RF Inductors - SMD 47 NH
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Murata 10024
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AUD 0.1155
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded47 nH2 %440 mA648 mOhms-- 55 C+ 125 C253.2 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQG15HS5N1B02D


RF Inductors - SMD 5.1 NH +-.1NH
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Murata 10010
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AUD 0.0273
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Multilayer0402 (1005 METRIC)Unshielded5.1 nH0.1 nH650 mA180 mOhms-- 55 C+ 125 C85.3 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQW15AN3N3C10D


RF Inductors - SMD Fixed IND 3.3nH 900mA NONAUTO
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Murata 10010
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AUD 0.0355
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Wirewound0402 (1005 METRIC)Unshielded3.3 nH 900 mA40 mOhms-- 55 C+ 125 C3012 GHzStandard1 mm0.5 mm0.5 mm-  LQW15AN_10Reel , Cut Tape
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