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
  
                         
NLCV32T-470K-EF


RF Inductors - SMD 47uH 2.132ohms 180mA Wound Ferrite
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TDK 9583
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AUD 0.0654
Multiples of: 10

Wirewound1210 (3225 METRIC)Unshielded47 uH10 %180 mA1.64 Ohms-- 40 C+ 105 C1514 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFReel , Cut Tape
NLV32T-221J-EF


RF Inductors - SMD 220uH 21ohms 50mA Wound Ferrite
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TDK 5257
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AUD 0.0556
Multiples of: 10

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded220 uH5 %50 mA21 Ohms-- 40 C+ 105 C207 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
NLFV32T-681K-EF


RF Inductors - SMD 3.2mm x 2.5mm x 2.2mm, -40 to +105 degC, 25mA, 680?H, 22.2ohm
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TDK 1818
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AUD 0.1354
Multiples of: 5

Wirewound1210 (3225 METRIC)Shielded680 uH10 %25 mA18.5 Ohms-- 40 C+ 105 C--Standard3.2 mm2.5 mm2.2 mm-Ferrite NLFV32 - EFReel , Cut Tape
AISC-0805-R12J-T


RF Inductors - SMD FIXED IND 120NH 400MA 510 MOHM
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ABRACON 1715
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AUD 0.3086
Multiples of: 1

Wirewound0805 (2317 METRIC)Unshielded120 nH5 %400 mA510 mOhms - 40 C+ 125 C501.1 GHzStandard2.29 mm1.73 mm1.55 mm Ceramic AISC - 0805Reel , Cut Tape
AL05A3N85GTR


RF Inductors - SMD 3.85nH 2% AIR CORE
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Kyocera AVX 1713
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AUD 0.3965
Multiples of: 1

Wirewound1.42 mm x 1.37 mm x 2.21 mmUnshielded3.85 nH2 %1.6 A6 mOhms-- 40 C+ 125 C1007.5 GHzStandard2.21 mm1.42 mm1.37 mm-Air ALReel , Cut Tape
MLF1608A3R3KTD25


RF Inductors - SMD 3.3uH 1.3ohms 30mA +/-10% Fer AEC-Q200
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TDK 1698
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AUD 0.1433
Multiples of: 1

Multilayer0603 (1608 METRIC)Shielded3.3 uH10 %30 mA1.3 Ohms-- 55 C+ 125 C35100 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
0402F-078K-08


Wire-wound Ferrite RF Chip
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Fastron 1697
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AUD 0.3315
Multiples of: 1000

                     
AISC-Q1008-123G-T


RF Inductors - SMD IND 12000nH 0.13A 10500m?
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Abracon 1694
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AUD 0.2348
Multiples of: 1

Ceramic Wirewound RF Inductor1008 (2928 METRIC)Unshielded12 uH2 %130 mA10.5 Ohms - 40 C+ 125 C1518 MHzStandard2.92 mm2.79 mm2.13 mm   AISC - Q1008Reel , Cut Tape
MLG1005S3N0BTD25


RF Inductors - SMD IND 0402 3.0nH StdQ AEC Q200 RF IND
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TDK 1649
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AUD 0.0125
Multiples of: 50

Multilayer0402 (1005 METRIC)Unshielded3 nH0.1 nH800 mA200 mOhms-- 55 C+ 125 C76.8 GHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
AIMC-0603-R18J-T


RF Inductors - SMD FIXED IND 180NH 300MA 1.8 OHM
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ABRACON 0
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AUD 0.0655
Multiples of: 1

Multilayer Ceramic Chip Inductor0603 (1608 METRIC)Shielded180 nH5 %200 mA1.9 Ohms - 55 C+ 125 C15400 MHzStandard1.6 mm0.8 mm0.8 mm Ceramic AIMC - 0603Reel , Cut Tape
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