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
  
                         
ISC1812ER1R8K


RF Inductors - SMD 1.8uh 10%
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Vishay 1455
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.5105

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Molded1812 (4532 METRIC)    15 mOhms     Standard      ISCReel , Cut Tape
IMC1812ER390J


RF Inductors - SMD 39uh 5%
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Vishay 1455
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.7108

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Molded1812 (4532 METRIC) 39 uH  15 mOhms     Standard      IMCReel , Cut Tape
PM105SB-221K-RC


Inductor Power Shielded Bobbin Core 220uH 10% 100KHz 27Q-Factor Ferrite 470mA 780mOhm DCR T/R
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Bourns 1455
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between Tue. 25 Nov to Mon. 01 Dec
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AUD 0.8333

Multiples of: 1

Wirewound Shielded220 uH20 %470 mA780 mOhms-- 30 C+ 100 C275 MHzStandard4.5 mm--9.9 mmFerrite PM105SBReel , Cut Tape
1812R-274J


RF Inductors - SMD 270uH 5%
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API Delevan 1455
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 2.3479

Multiples of: 1

Unshielded Surface Mount Inductors1812 (4532 METRIC)Unshielded270 uH5 %129 mA12 Ohms - 55 C+ 125 C404 MHz 4.83 mm3.4 mm3.4 mm Ferrite 1812RReel
S1812R-682K


RF Inductors - SMD 6.8uH 10%
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API Delevan 1455
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 4.0142

Multiples of: 1

RF Choke1812 (4532 METRIC)Shielded6.8 uH10 %408 mA1.2 Ohms-- 55 C+ 125 C4032 MHzStandard4.8 mm3.4 mm3.4 mm-Ferrite S1812/RReel , Cut Tape
B82432C1102K


RF Inductors - SMD SMT-INDUCTOR 1812 1 UH 10%, AEC-Q200
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TDK 1454
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.6078

Multiples of: 1

Wirewound1812 (4532 METRIC)Unshielded1 uH10 %600 mA280 mOhms-- 55 C+ 150 C40200 MHzStandard4.5 mm3.2 mm3.2 mm-FerriteAEC - Q200B82432CReel , Cut Tape
NLV32T-015J-EF


RF Inductors - SMD 15nH 160mohms 450mA Wound Ferrite
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TDK 1446
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1382

Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded15 nH5 %450 mA160 mOhms-- 40 C+ 105 C192.1 GHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
0805AS-082J-01


RF Inductors - SMD 82nH 150 MHz 5% Tol
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Fastron 1445
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1955

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded82 nH5 %400 mA420 mOhms-- 40 C+ 150 C671.3 GHzStandard2.3 mm1.8 mm1.6 mm-CeramicAEC - Q2000805ASReel , Cut Tape
LBM2016T3R3JV


RF Inductors - SMD 0806 3.3uH 5%
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Taiyo Yuden 1443
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1818

Multiples of: 1

Wirewound0806 (2016 METRIC)Unshielded3.3 uH5 %290 mA680 mOhms-- 40 C+ 105 C3048 MHzStandard2 mm1.6 mm1.6 mm-  LBMReel , Cut Tape
LQW18AN3N9D10D


RF Inductors - SMD
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Murata 1392
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.0934

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded3.9 nH0.5 nH1 A32 mOhms-- 55 C+ 125 C3811 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
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