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
  
                         
LQW15AN2N2D10D


RF Inductors - SMD 2.2 NH
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Murata 19400
Ships to you
between Thu. 09 Jul to Wed. 15 Jul
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AUD 0.0838

Multiples of: 10000

Wirewound0402 (1005 METRIC)Unshielded2.2 nH0.5 nH1 A27 mOhms-- 55 C+ 125 C2514 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
NLCV32T-1R0M-EF


RF Inductors - SMD INDUCTOR-COIL FXD 1UH +-20%
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TDK 8875
Ships to you
between Thu. 23 Jul to Tue. 28 Jul
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AUD 0.0563

Multiples of: 10

Wirewound1210 (3225 METRIC)Unshielded1 uH20 %1 A60 mOhms-- 40 C+ 105 C10100 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFReel , Cut Tape
B82498F3330J


RF Inductors - SMD 33nH 600mA 5% 2x1.3mm SMD
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TDK 4148
Ships to you
between Thu. 09 Jul to Wed. 15 Jul
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AUD 0.1328

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded33 nH5 %600 mA110 mOhms-- 55 C+ 125 C652.2 GHzStandard2 mm1.3 mm1.4 mm-Ceramic B82498FReel , Cut Tape
WCLA2520V1-100-R


RF Inductors - SMD Chip IND 10.0uH 0.392A SMT 2 Pad
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Eaton 4145
Ships to you
between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.2514

Multiples of: 1

Wirewound1008 (2520 METRIC)Shielded10 uH10 %392 mA860 mOhms - 55 C+ 125 C1228 MHz 2.9 mm2.5 mm2.1 mm Ferrite WCLAReel , Cut Tape
LQW2BASR12G00L


RF Inductors - SMD 120 NH 2%
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Murata 4140
Ships to you
between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.131

Multiples of: 1

Wirewound0805 (2015 METRIC)Unshielded120 nH2 %400 mA510 mOhms-- 55 C+ 125 C501.1 GHzStandard2.09 mm1.53 mm1.42 mm-- LQW2BAReel , Cut Tape
MCQ1V2012-1R5-R


RF Inductors - SMD Multi H Q, IND 1.5uH Q35 50mA 2PADS SMT
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Eaton 4139
Ships to you
between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.0258

Multiples of: 1

Multilayer0805 (2012 METRIC)Unshielded1.5 uH10 %50 mA400 mOhms-- 40 C+ 85 C3560 MHzStandard2 mm1.2 mm0.9 mm-  MCQ1VReel , Cut Tape
MLG0603P6N8JTD25


RF Inductors - SMD IND 0201 6.8nH Hi-Q AEC Q200 RF IND
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TDK 4138
Ships to you
between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.0309

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded6.8 nH5 %300 mA750 mOhms-- 55 C+ 125 C146.1 GHzStandard0.6 mm0.3 mm0.3 mm-CeramicAEC - Q200MLG - PReel , Cut Tape
MLF2012DR22JTD25


RF Inductors - SMD 220nH 300mohms 250mA +/-5% Fer AEC-Q200
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TDK 4131
Ships to you
between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.1499

Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded220 nH5 %250 mA300 mOhms-- 55 C+ 125 C20330 MHzStandard2 mm1.25 mm0.85 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQW15AN3N4D80D


RF Inductors - SMD
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 4119
Ships to you
between Wed. 15 Jul to Fri. 17 Jul
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AUD 0.1131

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded3.4 nH0.5 nH1.95 A30 mOhms-- 55 C+ 125 C3010 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQW15AN4N3G80D


Inductors (SMD) 0402 RoHS
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 2643
Ships to you
between Thu. 23 Jul to Tue. 28 Jul
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AUD 0.0698

Multiples of: 5

Wirewound0402 (1005 METRIC)Unshielded4.3 nH2 %1.8 A44 mOhms-- 55 C+ 125 C329.6 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
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