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
  
                         
NLV32T-101J-EFD


RF Inductors - SMD 100uH 10ohms 40mA Wound Fer AEC-Q200
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TDK 1615
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between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.1276

Multiples of: 5

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded100 uH5 %40 mA10 Ohms-- 40 C+ 105 C2010 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
AISC-1008-R33G-T


RF Inductors - SMD FIXED IND 330NH 450MA 1.05 OHM
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ABRACON 1574
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.3025

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Wirewound1008 (2520 METRIC)Unshielded330 nH2 %450 mA1.05 Ohms - 40 C+ 125 C50530 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
PM0805-5N6M-RC


RF Inductors - SMD 5.6uH 20%
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Bourns 1562
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.224

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Wirewound0805 (2012 METRIC)Unshielded5.6 nH20 %600 mA55 Ohms-- 55 C+ 125 C605.8 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic PM0805Reel , Cut Tape
LQW2BANR11G00L


RF Inductors - SMD
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Murata 1561
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between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.1562

Multiples of: 5

Wirewound0805 (2015 METRIC)Unshielded110 nH2 %970 mA380 mOhms-- 55 C+ 125 C571.2 GHzStandard2.09 mm1.53 mm1.42 mm-  LQW2BAReel , Cut Tape
LQG18HHR10J00D


RF Inductors - SMD 100 NH +-.3NH
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Murata 1556
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1595

Multiples of: 1

Multilayer0603 (1608 METRIC)Unshielded100 nH5 %300 mA900 mOhms-- 55 C+ 125 C12600 MHzStandard1.6 mm0.8 mm0.8 mm-AirAEC - Q200LQGReel , Cut Tape
LBM2016T390J


RF Inductors - SMD 963-LSQMB201616T390J RPLCMT PN 0806 39uH 5070mOhms 5% 120mA
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Taiyo Yuden 1555
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.0953

Multiples of: 1

Wirewound0806 (2016 METRIC)Unshielded39 uH5 %120 mA5.07 Ohms-- 40 C+ 105 C2014 MHzStandard2 mm1.6 mm1.8 mm-  LBMReel , Cut Tape
MLF1608A1R0KTA00


Inductor RF Chip Shielded Multi-Layer 1uH 10% 10MHz 35Q-Factor Ferrite 50mA 500mOhm DCR 0603 T/R
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TDK 1552
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AUD 0.043

Multiples of: 20

Multilayer0603 (1608 METRIC)Shielded1 uH10 %50 mA500 mOhms-- 55 C+ 125 C35170 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
S1210R-393K


RF Inductors - SMD 39uH 10%
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API Delevan 1547
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AUD 3.0693

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Wirewound1210 (3225 METRIC)Shielded39 uH10 %179 mA5 Ohms-- 55 C+ 125 C4012 MHzStandard3.51 mm2.66 mm2.57 mm-Ferrite S1210/RReel , Cut Tape
MHQ0603P3N6CT000


RF Inductors - SMD IND 0201 3.6nH S-HQ SMD RF IND
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TDK 1546
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AUD 0.0667

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded3.6 nH0.2 nH500 mA250 mOhms-- 55 C+ 125 C169.1 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
NLV25T-2R2J-EF


RF Inductors - SMD 2.2uH 1.55ohms 200mA Wound Ferrite
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TDK 1367
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between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.0556

Multiples of: 10

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded2.2 uH5 %200 mA1.55 Ohms-- 40 C+ 105 C30105 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
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