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
  
                         
AISC-0402-3N6J-T


RF Inductors - SMD FIXED IND 3.6NH 840MA 66 MOHM
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ABRACON 3614
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AUD 0.1296
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Smd Ceramic Wire - Wound Chip Inductors0402 (1005 METRIC)Unshielded3.6 nH5 %840 mA66 mOhms - 40 C+ 125 C206800 MHz 1.19 mm0.64 mm0.66 mm Ceramic Aisc - 0402Reel
LQW2UASR18G00L


RF Inductors - SMD .18 UH 2%
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Murata 3612
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AUD 0.1614
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Wirewound1008 (2520 METRIC)Unshielded180 nH2 %620 mA770 mOhms-- 55 C+ 125 C45750 MHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
B82432C1682K000


RF Inductors - SMD 1812 6.8uH 10%
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TDK 3612
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AUD 0.7168
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Wirewound1812 (4532 METRIC)Unshielded6.8 uH10 %360 mA780 mOhms-- 55 C+ 150 C4035 MHzStandard4.5 mm3.2 mm3.2 mm-FerriteAEC - Q200B82432CReel , Cut Tape
LQW18AS22NG0ZD


RF Inductors - SMD
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Murata 3611
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AUD 0.1079
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Wirewound0603 (1608 METRIC)Unshielded22 nH2 %700 mA190 mOhms-- 40 C+ 125 C383 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
MLF2012D82NMTD25


RF Inductors - SMD 82nH 150mohms 300mA +/-20% Fer AEC-Q200
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TDK 3611
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AUD 0.1193
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Multilayer0805 (2012 METRIC)Shielded82 nH20 %300 mA150 mOhms-- 55 C+ 125 C15550 MHzStandard2 mm1.25 mm0.85 mm-FerriteAEC - Q200MLFReel , Cut Tape
NLV32T-R47J-EF


RF Inductors - SMD 470nH 500mohms 450mA Wound Ferrite
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TDK 3608
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AUD 0.0583
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Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded470 nH5 %450 mA500 mOhms-- 40 C+ 105 C30220 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
MLF1608A3R9MTD25


RF Inductors - SMD 3.9uH 1.45ohms 30mA +/-20% Fer AEC-Q200
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TDK 3608
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AUD 0.1287
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Multilayer0603 (1608 METRIC)Shielded3.9 uH20 %30 mA1.45 Ohms-- 55 C+ 125 C3590 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
LBM2016T120J


RF Inductors - SMD 963-LSQMB201616T120J RPLCMT PN 0806 12uH 1820mOhms 5% 200mA
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Taiyo Yuden 3606
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AUD 0.0953
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Wirewound0806 (2016 METRIC)Unshielded12 uH5 %200 mA1.82 Ohms-- 40 C+ 105 C2523 MHzStandard2 mm1.6 mm1.8 mm-  LBMReel , Cut Tape
B82422A3220K100


RF Inductors - SMD 22nH 600mA 10% 1210 SMD, AEC-Q200
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TDK 3601
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AUD 0.3124
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Wirewound1210 (3225 METRIC)Unshielded22 nH10 %600 mA140 mOhms-- 55 C+ 145 C302.5 GHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422AReel , Cut Tape
LQG15HH5N6S02D


RF Inductors - SMD
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Murata 3600
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AUD 0.1004
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Multilayer0402 (1005 METRIC)Unshielded5.6 nH0.3 nH650 mA180 mOhms-- 55 C+ 125 C84.5 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
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