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
  
                         
NLV32T-560J-EFD


RF Inductors - SMD 56uH 8.0ohms 55mA Wound Fer AEC-Q200
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TDK 1536
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AUD 0.1552
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Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded56 uH5 %55 mA8 Ohms-- 40 C+ 105 C3013 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
MCLA1608V2-181-R


RF Inductors - SMD MCLA Auto Chip IND 1608 180nH 2 Pads
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Eaton 216
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AUD 0.0483
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Multilayer0603 (1608 METRIC)Unshielded180 nH5 %200 mA1.9 Ohms-- 40 C+ 125 C8400 MHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200MCLAReel , Cut Tape
LQW15AN3N4C10D


RF Inductors - SMD
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Murata 213
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AUD 0.0569
Multiples of: 10

Wirewound0402 (1005 METRIC)Unshielded3.4 nH0.2 nH900 mA40 mOhms-- 55 C+ 125 C3012 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
4310LC-352KEC


RF Inductors - SMD 4310 3.5uH Unshld 10% 49mOhms
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Coilcraft 212
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AUD 3.7848
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Wideband Bias Choke4.826 mm x 3.3 mm x 11.68 mmUnshielded3.5 uH10 %3.1 A49 mOhms-- 40 C+ 85 C-188 MHzStandard11.68 mm4.826 mm3.3 mm-Ferrite 4310LCReel , Cut Tape
1210R-331K


RF Inductors - SMD 0.33uH 10%
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API Delevan 212
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AUD 1.9202
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Wirewound1210 (3225 METRIC)Unshielded330 nH10 %720 mA400 mOhms-- 55 C+ 125 C30300 MHzStandard3.51 mm2.67 mm2.57 mm-Iron 1210/RReel , Cut Tape
1111SQ-39NGEC


RF Inductors - SMD 1111 39nH Unshld 2% 4.8A 10mOhms
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Coilcraft 199
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AUD 1.4852
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Wirewound2.67 mm x 2.79 mm x 2.92 mmUnshielded39 nH2 %4.8 A10 mOhms-- 40 C+ 125 C2002.2 GHzStandard2.92 mm2.67 mm2.79 mm-Air 1111SQReel , Cut Tape
LQW2BAS91NG00L


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 198
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AUD 0.131
Multiples of: 1

Wirewound0805 (2015 METRIC)Unshielded91 nH2 %400 mA480 mOhms-- 55 C+ 125 C651.33 GHzStandard2.09 mm1.53 mm1.42 mm-  LQW2BAReel , Cut Tape
MHQ1005P18NGT000


RF Inductors - SMD IND 0402 18nH S-HQ SMD RF IND
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TDK 155
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AUD 0.0252
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Multilayer0402 (1005 METRIC)Unshielded18 nH2 %260 mA800 mOhms-- 55 C+ 125 C223.4 GHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
AISC-1008-R27J-T


RF Inductors - SMD FIXED IND 270NH 500MA 910 MOHM
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ABRACON 155
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AUD 0.2858
Multiples of: 5

Wirewound1008 (2520 METRIC)Unshielded270 nH5 %500 mA910 mOhms - 40 C+ 125 C50600 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
B82422-A1222-K100


RF Inductors - SMD 2.2uH 270mA 10% 1210 SMD, AEC-Q200
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TDK 38
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AUD 0.2226
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Wirewound1210 (3225 METRIC)Unshielded2.2 uH10 %270 mA750 mOhms-- 55 C+ 145 C25125 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
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