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
  
                         
AWCS00231715R47J00


RF Inductors - SMD Chilisin RF inductor Wire Wound-STD
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Pulse 1940
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AUD 0.1448
Multiples of: 1

 2.35 mm x 1.73 mm x 1.52 mmUnshielded470 nH5 %250 mA1.76 Ohms - 40 C+ 125 C33450 MHzStandard2.35 mm1.73 mm1.52 mm  AEC - Q200AWCSReel , Cut Tape
MLF2012C150KTD25


RF Inductors - SMD 15uH 700mohms 5mA +/-10% Fer AEC-Q200
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TDK 1940
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AUD 0.1535
Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded15 uH10 %5 mA700 mOhms-- 55 C+ 125 C3040 MHzStandard2 mm1.25 mm1.25 mm-FerriteAEC - Q200MLFReel , Cut Tape
MLF2012E120JTD25


RF Inductors - SMD 12uH 900mohms 15mA +/-5% Fer AEC-Q200
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TDK 1940
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AUD 0.163
Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded12 uH5 %15 mA900 mOhms-- 55 C+ 125 C5045 MHzStandard2 mm1.25 mm1.25 mm-FerriteAEC - Q200MLFReel , Cut Tape
AISC-1008-1R0G-T


RF Inductors - SMD FIXED IND 1UH 370MA 1.8 OHM SMD
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ABRACON 1940
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AUD 0.1705
Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded1 uH2 %370 mA1.8 Ohms - 40 C+ 125 C35270 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
NLFV25T-4R7M-EF


RF Inductors - SMD 4.7uH 290mohms 210mA Wound Ferrite
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TDK 1940
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AUD 0.1705
Multiples of: 1

Wirewound2.5 mm x 2 mm x 1.8 mmShielded4.7 uH20 %210 mA240 mOhms-- 40 C+ 105 C--Standard2.5 mm2 mm1.8 mm-Ferrite NLFV25 - EFReel , Cut Tape
AISC-1210HS-330K-T2


RF Inductors - SMD 33000NH 10% -40C +85C
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ABRACON 1940
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AUD 0.1754
Multiples of: 2000

Wirewound1210 (3225 METRIC)Unshielded33 uH10 %220 mA5 Ohms250 mA- 40 C+ 85 C1020 MHzStandard3.2 mm3.05 mm1.3 mm Ferrite AISC - 1210HSReel , Cut Tape
AISC-1210HS-3R3K-T2


RF Inductors - SMD FIXED IND 3.3UH 650MA 750 MOHM
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ABRACON 1940
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AUD 0.1874
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded3.3 uH10 %650 mA750 mOhms700 mA- 40 C+ 85 C10100 MHzStandard3.2 mm3.05 mm1.3 mm Ferrite AISC - 1210HSReel , Cut Tape
1008AS-010J-01


RF Inductors - SMD 10nH 50 MHz 5% Tol
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Fastron 1940
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AUD 0.1895
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Wirewound1008 (2520 METRIC)Unshielded10 nH5 %1 A80 mOhms-- 40 C+ 125 C504.1 GHzStandard2.9 mm2.8 mm2.1 mm-CeramicAEC - Q2001008ASReel , Cut Tape
NLV32T-068J-EFD


RF Inductors - SMD 68nH 360mohms 450mA Wound Fer AEC-Q200
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TDK 1940
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AUD 0.1925
Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded68 nH5 %450 mA360 mOhms-- 40 C+ 105 C271 GHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
0805AS-R56J-08


RF Inductors - SMD Wire-wound Ceramic RF Chip Inductor
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Fastron 1940
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AUD 0.2138
Multiples of: 1000

Wirewound0805 (2012 METRIC)Unshielded560 nH5 %170 mA3.5 Ohms-- 40 C+ 150 C40650 MHzStandard2.3 mm1.8 mm1.6 mm-CeramicAEC - Q2000805ASReel , Cut Tape
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