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
  
                         
AIML-0603-4R7K-T


RF Inductors - SMD 4.7 UH +/-10%
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ABRACON 44253
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AUD 0.0379
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Multilayer0603 (1608 METRIC)Shielded4.7 uH10 %15 mA2.1 Ohms - 55 C+ 125 C3550 MHzStandard1.6 mm0.8 mm0.8 mm Ferrite AIML - 0603Reel , Cut Tape
LQW15AN18NG8ZD


RF Inductors - SMD 18 NH 2%
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Murata 43167
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AUD 0.1072
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Wirewound0402 (1005 METRIC)Unshielded18 nH2 %1.05 A130 mOhms-- 55 C+ 125 C305.2 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LCCI0201S5N6GTAR


RF Inductors - SMD 5.6nH Tol 0.3nH 0201 350mA DCR=.4 Ohms
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Kyocera AVX 43160
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AUD 0.0162
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Multilayer0201 (0603 METRIC)Unshielded5.6 nH0.3 nH350 mA400 mOhms-- 40 C+ 85 C56 GHzStandard0.6 mm0.3 mm0.3 mm-  LCCIReel , Cut Tape
LCCI0201S2N2GTAR


RF Inductors - SMD 2.2nH Tol 0.3nH 0201 450mA DCR=.22 Ohms
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Kyocera AVX 42937
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AUD 0.0101
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Multilayer0201 (0603 METRIC)Unshielded2.2 nH0.3 nH450 mA220 mOhms-- 40 C+ 85 C410 GHzStandard0.6 mm0.3 mm0.3 mm-  LCCIReel , Cut Tape
BWCM0012070715NG00


RF Inductors - SMD 15nH RDC=0.16Ohms 460mA
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Pulse 42655
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AUD 0.0974
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 1.6 mm x 0.7 mm x 0.66 mmUnshielded15 nH2 %460 mA160 mOhms460 mA- 55 C+ 125 C305 GHzStandard1.2 mm0.7 mm0.66 mm-Ceramic BWCMReel , Cut Tape
LQP03TQ3N0C02D


RF Inductors - SMD 3nH 500mA 0201 (0603 metric) SUGGESTED ALT LQP03HQ3N0C02D
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Murata 42597
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AUD 0.0273
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Thin Film0201 (0603 METRIC)Unshielded3 nH0.2 nH500 mA200 mOhms - 55 C+ 125 C179.5 GHzStandard0.6 mm0.3 mm0.3 mm Ferrite LQPReel , Cut Tape
LQP03TG1N9B02D


RF Inductors - SMD
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 42513
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AUD 0.0148
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Thin Film0201 (0603 METRIC)Unshielded1.9 nH0.1 nH450 mA250 mOhms - 55 C+ 125 C1312.5 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP02TN1N3B02D


RF Inductors - SMD
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Murata 42456
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AUD 0.0485
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Thin Film01005 (0402 METRIC)Unshielded1.3 nH0.1 nH220 mA600 mOhms - 55 C+ 125 C811.5 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
CIGT201610LH1R0MNE


RF Inductors - SMD CIGT,Thin Film,0806,1.0uH,1.0?,7 embossed,-20 20%
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SAMSUNG 40832
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AUD 0.0943
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Thin Film  1 uH20 %              CIGTReel , Cut Tape
CIGT252010TM1R0MLE


RF Inductors - SMD 1uH, +/-20%, 1008, L Type, TH, in Film
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SAMSUNG 39100
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AUD 0.2703
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Wirewound1008 (2520 METRIC)Shielded1 uH20 %5 A23 mOhms5.3 A- 40 C+ 125 C  Standard2.5 mm2 mm1 mm Metal  Reel , Cut Tape
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