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
  
                         
LQW18AN3N9C00D


RF Inductors - SMD 3.9 NH +-.2NH
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Murata 8885
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AUD 0.0434
Multiples of: 10

Wirewound0603 (1608 METRIC)Unshielded3.9 nH0.2 nH850 mA59 mOhms-- 55 C+ 125 C356 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
B82422-A1222-K100


RF Inductors - SMD 2.2uH 270mA 10% 1210 SMD, AEC-Q200
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TDK 1227
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AUD 0.2761
Multiples of: 5

Wirewound1210 (3225 METRIC)Unshielded2.2 uH10 %270 mA750 mOhms-- 55 C+ 145 C25125 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
1812R-122J


RF Inductors - SMD 1.2uH 5%
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API Delevan 1212
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AUD 2.3767
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Molded1812 (4532 METRIC)Unshielded1.2 uH5 %604 mA550 mOhms-- 55 C+ 125 C5080 MHzStandard4.83 mm3.4 mm3.4 mm-Ferrite 1812/RReel , Cut Tape
AISC-0805F-6R8J-T


RF Inductors - SMD Inductor Ceramic Core Wire wound 2.3 x 1.7 x 1.55mm
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ABRACON 1208
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AUD 0.2512
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Wirewound0805 (2012 METRIC)Unshielded6.8 uH5 %115 mA3.4 Ohms - 40 C+ 125 C1536 MHzStandard2.29 mm1.73 mm1.55 mm Ferrite AISC - 0805FReel , Cut Tape
B82498F3829K


RF Inductors - SMD 8.2nH 700mA 10% 2.3x1.7mm SMD
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TDK 1205
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AUD 0.3852
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Wirewound0805 (2012 METRIC)Unshielded8.2 nH10 %700 mA90 mOhms-- 55 C+ 125 C505 GHzStandard2 mm1.3 mm1.4 mm-Ceramic B82498FReel , Cut Tape
AIML-0805-1R2K-T


RF Inductors - SMD FIXED IND 1.2UH 50MA 500 MOHM
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ABRACON 1197
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AUD 0.0789
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Multilayer Ferrite Chip Inductor0805 (2012 METRIC)Shielded1.2 uH10 %50 mA500 mOhms - 55 C+ 125 C4585 MHzStandard2 mm1.25 mm0.85 mm Ferrite AIML - 0805Reel , Cut Tape
NLV25T-270J-EFD


RF Inductors - SMD 27uH 6.3ohms 115mA Wound Fer AEC-Q200
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TDK 1196
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AUD 0.1614
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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded27 uH5 %115 mA6.3 Ohms-- 40 C+ 105 C2521 MHzStandard2.5 mm2 mm1.8 mm-FerriteAEC - Q200NLV25 - EFDReel , Cut Tape
LQP03HQ2N9B02D


RF Inductors - SMD 2.9 NH +/-0.1NH
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Murata 1183
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AUD 0.0367
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Thin Film0201 (0603 METRIC)Unshielded2.9 nH0.1 nH600 mA120 mOhms-- 55 C+ 125 C208 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
NLV25T-R68J-EF


RF Inductors - SMD 680nH 850mohms 300mA Wound Ferrite
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TDK 1115
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AUD 0.0531
Multiples of: 10

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded680 nH5 %300 mA850 mOhms-- 40 C+ 105 C30300 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
NLV25T-101J-EFD


RF Inductors - SMD 100uH 21ohms 60mA Wound Fer AEC-Q200
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TDK 0
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AUD 0.1614
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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded100 uH5 %60 mA21 Ohms-- 40 C+ 105 C1512 MHzStandard2.5 mm2 mm1.8 mm-FerriteAEC - Q200NLV25 - EFDReel , Cut Tape
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