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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Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
LQW15AN3N0D8ZD


RF Inductors - SMD
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Murata 10822
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between Mon. 20 Jul to Wed. 22 Jul
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AUD 0.1051

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Wirewound0402 (1005 METRIC)Unshielded3 nH0.5 nH1.35 A63 mOhms-- 55 C+ 125 C2012.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LQW18AN8N7C00D


RF Inductors - SMD
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Murata 5009
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AUD 0.0827

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Wirewound0603 (1608 METRIC)Unshielded8.7 nH0.2 nH650 mA110 mOhms-- 55 C+ 125 C356 GHzStandard1.6 mm0.8 mm0.95 mm-  LQWReel , Cut Tape
PE-0603CD221GTT


RF Inductors - SMD 220nH 2%
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Pulse 1628
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between Mon. 20 Jul to Wed. 22 Jul
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AUD 0.2844

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Multilayer0603 (1608 METRIC)Unshielded220 nH2 %200 mA1.9 Ohms-- 40 C+ 125 C25900 MHzStandard1.8 mm1.24 mm1.02 mm-Ceramic CDReel , Cut Tape
PM0603-39NJ-RC


Inductor Chip Wirewound 39nH 5% 250MHz 35Q-Factor Alumina 600mA 250mOhm DCR 0603 T/R
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Bourns 1142
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AUD 0.2724

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Wirewound0603 (1608 METRIC)Unshielded39 nH5 %600 mA250 mOhms-- 40 C+ 125 C432.2 GHzStandard1.65 mm1.05 mm1 mm-Alumina PM0603Reel , Cut Tape
NLV32T-6R8J-EFD


RF Inductors - SMD 6.8uH 1.8ohms 180mA Wound Fer AEC-Q200
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TDK 1131
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AUD 0.1517

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Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded6.8 uH5 %180 mA1.8 Ohms-- 40 C+ 105 C3040 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
LQW2UASR56J00L


RF Inductors - SMD .56 UH 5%
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Murata 1130
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AUD 0.1114

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Wirewound1008 (2520 METRIC)Unshielded560 nH5 %400 mA1.33 Ohms-- 55 C+ 125 C45415 MHzStandard2.62 mm2.45 mm1.83 mm-Air LQWReel , Cut Tape
AISC-0805F-3R3J-T


RF Inductors - SMD Inductor Ceramic Core Wire wound 2.3 x 1.7 x 1.55mm
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ABRACON 1125
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AUD 0.2379

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Wirewound0805 (2012 METRIC)Unshielded3.3 uH5 %175 mA2.3 Ohms - 40 C+ 125 C1550 MHzStandard2.29 mm1.73 mm1.55 mm Ferrite AISC - 0805FReel , Cut Tape
AISC-1210HS-220K-T2


RF Inductors - SMD FIXED IND 22UH 300MA 3.5 OHM SMD
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Abracon 1119
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AUD 0.1827

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Wirewound1210 (3225 METRIC)Unshielded22 uH10 %300 mA3.5 Ohms320 mA- 40 C+ 85 C1030 MHzStandard3.2 mm3.05 mm1.3 mm Ferrite AISC - 1210HSReel , Cut Tape
MLF1608DR27JT000


RF Inductors - SMD 1.6mm x 0.8mm x 0.8mm, -55 to +125 degC, 150mA, 0.27?H, 600mohm
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TDK 1092
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AUD 0.04

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Multilayer0603 (1608 METRIC)Shielded270 nH5 %150 mA600 mOhms-- 55 C+ 125 C15350 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
NLFV25T-680K-EF


RF Inductors - SMD 68uH 3.96ohms 50mA Wound Ferrite
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TDK 935
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between Mon. 20 Jul to Wed. 22 Jul
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AUD 0.1431

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Wirewound2.5 mm x 2 mm x 1.8 mmShielded68 uH10 %50 mA3.3 Ohms-- 40 C+ 105 C--Standard2.5 mm2 mm1.8 mm-Ferrite NLFV25 - EFReel , Cut Tape
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