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
  
                         
NLFV32T-330K-EF


RF Inductors - SMD 3.2mm x 2.5mm x 2.2mm, -40 to +105 degC, 95mA, 33?H, 780mohm
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TDK 3699
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AUD 0.2103
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Wirewound1210 (3225 METRIC)Shielded33 uH10 %95 mA650 mOhms-- 40 C+ 105 C--Standard3.2 mm2.5 mm2.2 mm-Ferrite NLFV32 - EFReel , Cut Tape
B82422A3181K100


RF Inductors - SMD SMT-INDUCTOR 1210 0.18UH 10%, AECQ200
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TDK 3696
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AUD 0.2861
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Wirewound1210 (3225 METRIC)Unshielded180 nH10 %360 mA380 mOhms-- 55 C+ 145 C25800 MHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422AReel , Cut Tape
BSCL00201209R82K00


RF Inductors - SMD Chilisin RF inductor Multilayer-STD
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Pulse 3695
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AUD 0.1037
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 2 mm x 1.25 mm x 0.9 mmShielded820 nH10 % 1 Ohms150 mA- 40 C+ 125 C25100 MHzStandard2 mm1.25 mm0.9 mm Ferrite BSCLReel , Cut Tape
HL02180GTTR


RF Inductors - SMD 18nH 2%
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Kyocera AVX 3689
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AUD 0.6442
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Multilayer Organic (MLO)0402 (1005 METRIC)Unshielded18 nH2 %85 mA1.5 Ohms-- 55 C+ 125 C153 GHzStandard1 mm0.58 mm0.35 mm-  HLReel , Cut Tape
LQW2UASR75F00L


RF Inductors - SMD
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Murata 3687
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AUD 0.3017
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Wirewound1008 (2520 METRIC)Unshielded750 nH1 %360 mA1.54 Ohms-- 55 C+ 125 C45360 MHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
LQG15HS1N1S02D


RF Inductors - SMD 1.1 NH +-.3NH
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Murata 3686
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AUD 0.0178
Multiples of: 50

Multilayer0402 (1005 METRIC)Unshielded1.1 nH0.3 nH1 A70 mOhms - 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
NLV32T-1R0J-EFD


RF Inductors - SMD 1.0uH 700mohms 400mA Wound Fer AEC-Q200
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TDK 3685
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AUD 0.1638
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Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded1 uH5 %400 mA700 mOhms-- 40 C+ 105 C30120 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
L0603100GGSTR


RF Inductors - SMD 10nH 2% 0603 SMD Hig h Q RF
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Kyocera AVX 3683
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AUD 0.5431
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Thin Film0603 (1608 METRIC)Unshielded10 nH2 %300 mA450 mOhms-- 55 C+ 125 C283.5 GHzStandard1.6 mm0.81 mm0.61 mm-  0603, 0805Reel , Cut Tape
CW201212-15NJ


RF Inductors - SMD 15nH 5%
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Bourns 3665
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AUD 0.1913
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Wirewound0805 (2012 METRIC)Unshielded15 nH5 %600 mA80 mOhms-- 40 C+ 125 C603.6 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW201212Reel , Cut Tape
LQG15HN2N2B02D


RF Inductors - SMD
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Murata 2728
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AUD 0.0465
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Multilayer0402 (1005 METRIC)Unshielded2.2 nH0.1 nH900 mA90 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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