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
  
                         
ILSB0805ER8R2K


RF Inductors - SMD 8.2uH 10%
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Vishay 4197
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1306

Multiples of: 1

Established Reliability0805 (2012 METRIC)Shielded8.2 uH10 %15 mA1.1 Ohms-- 55 C+ 125 C4530 MHzStandard2 mm1.25 mm1.25 mm-  ILSB - 0805Reel , Cut Tape
B82498F3100J


RF Inductors - SMD 10nH 700mA 5% 2x1.3mm SMD
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TDK 4187
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3863

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded10 nH5 %700 mA90 mOhms-- 55 C+ 125 C505 GHzStandard2 mm1.3 mm1.4 mm-Ceramic B82498FReel , Cut Tape
LQW18AS33NG0CD


RF Inductors - SMD Fixed IND 33nH 600mA NONAUTO
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Murata 4186
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2898

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded33 nH2 %600 mA220 mOhms-- 55 C+ 125 C402.3 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
CW201212-22NJ


Inductor RF Wirewound 0.022uH 5% 250MHz 55Q-Factor Ceramic 0.5A 0.22Ohm DCR 0805 T/R
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Bourns 4185
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1944

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded22 nH5 %600 mA100 mOhms-- 40 C+ 125 C603.3 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW201212Reel , Cut Tape
MLF2012A1R8KTD25


RF Inductors - SMD 1.8uH 450mohms 80mA +/-10% Fer AEC-Q200
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TDK 4181
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1302

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Multilayer0805 (2012 METRIC)Shielded1.8 uH10 %80 mA450 mOhms-- 55 C+ 125 C45130 MHzStandard2 mm1.25 mm0.85 mm-FerriteAEC - Q200MLFReel , Cut Tape
ILSB1206ER1R8K


RF Inductors - SMD 1.8uH 10%
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Vishay 4179
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1287

Multiples of: 1

Established Reliability1206 (3216 METRIC)Shielded1.8 uH10 %50 mA500 mOhms-- 55 C+ 125 C4564 MHzStandard3.2 mm1.6 mm1.1 mm-  ILSB - 1206Reel , Cut Tape
LBM2016T1R8J


RF Inductors - SMD 963-LSQMB201616T1R8J RPLCMT PN 0806 1.8uH 624mOhms 5% 345mA
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Taiyo Yuden 4163
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0953

Multiples of: 1

Wirewound0806 (2016 METRIC)Unshielded1.8 uH5 %345 mA624 mOhms-- 40 C+ 105 C30100 MHzStandard2 mm1.6 mm1.8 mm-  LBMReel , Cut Tape
NLV32T-4R7J-EF


RF Inductors - SMD 4.7uH 1.5ohms 220mA Wound Ferrite
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TDK 4083
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0497

Multiples of: 10

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded4.7 uH5 %220 mA1.5 Ohms-- 40 C+ 105 C3050 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
MLG1005S33NJT000


RF Inductors - SMD IND 0402 33nH StdQ SMD RF IND
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TDK 3783
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.009

Multiples of: 50

Multilayer0402 (1005 METRIC)Unshielded33 nH5 %300 mA900 mOhms-- 55 C+ 125 C81.8 GHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , Cut Tape
NLV32T-180J-EF


RF Inductors - SMD 18uH 3.3ohms 120mA Wound Ferrite
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TDK 2104
Ships to you
between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0585

Multiples of: 10

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded18 uH5 %120 mA3.3 Ohms-- 40 C+ 105 C3020 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
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