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
  
                         
WCLA2520V1-100-R


RF Inductors - SMD Chip IND 10.0uH 0.392A SMT 2 Pad
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Eaton 4413
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.2305

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Wirewound1008 (2520 METRIC)Shielded10 uH10 %392 mA860 mOhms - 55 C+ 125 C1228 MHz 2.9 mm2.5 mm2.1 mm Ferrite WCLAReel , Cut Tape
LQW18AN83NG80D


RF Inductors - SMD
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Murata 4403
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.1131

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded83 nH2 %550 mA500 mOhms-- 55 C+ 125 C342.23 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
B82432C1683K000


RF Inductors - SMD SMT-INDUCTOR 1812 68UH 10%, AEC-Q200
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TDK 4402
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.7168

Multiples of: 1

Wirewound1812 (4532 METRIC)Unshielded68 uH10 %190 mA2.8 Ohms-- 55 C+ 150 C3010 MHzStandard4.5 mm3.2 mm3.2 mm-FerriteAEC - Q200B82432CReel , Cut Tape
B82498F3181J000


RF Inductors - SMD SMT-INDUCTOR 0805 180NH 5%
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TDK 4383
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.3686

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Wirewound0805 (2012 METRIC)Unshielded180 nH5 %340 mA530 mOhms-- 55 C+ 125 C451.05 GHzStandard2 mm1.3 mm1.4 mm-Ceramic B82498FReel , Cut Tape
AIML-0805-R22K-T


RF Inductors - SMD FIXED IND 220NH 250MA 500 MOHM
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ABRACON 4373
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between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0789

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Multilayer Ferrite Chip Inductor0805 (2012 METRIC)Shielded220 nH10 %250 mA500 mOhms - 55 C+ 125 C20170 MHzStandard2 mm1.25 mm1.25 mm Ferrite AIML - 0805Reel , Cut Tape
LQP03TN0N7BZ2D


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 4372
Ships to you
between Thu. 27 Nov to Mon. 01 Dec
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AUD 0.0441

Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded700 pH0.1 nH800 mA80 mOhms-- 55 C+ 125 C1420 GHzStandard0.6 mm0.3 mm0.3 mm-FerriteAEC - Q200LQPReel , Cut Tape
LQW15AN12NH00D


RF Inductors - SMD 12 NH 3%
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Murata 4365
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.0405

Multiples of: 10

Wirewound0402 (1005 METRIC)Unshielded12 nH3 %500 mA140 mOhms-- 55 C+ 125 C305.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
NLCV32T-100K-EFRD


RF Inductors - SMD 10uH 0.42ohms 600mA 3.2x2.5mm AEC-Q200
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TDK 4345
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.1231

Multiples of: 5

Wirewound1210 (3225 METRIC)Unshielded10 uH10 %450 mA360 mOhms-- 40 C+ 105 C1530 MHzStandard3.2 mm2.5 mm2.4 mm-FerriteAEC - Q200NLCV - EFRDReel , Cut Tape
LQW18CNR65J0ZD


RF Inductors - SMD Fixed IND 650nH 430mA INFOTMT
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Murata 4166
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.1051

Multiples of: 5

Wirewound0603 (1608 METRIC)Unshielded650 nH5 %430 mA520 mOhms-- 55 C+ 125 C-510 MHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
Hot NLV32T-2R2J-EF


RF Inductors - SMD 2.2uH 1.0ohms 320mA Wound Ferrite
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TDK 814
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between Fri. 05 Dec to Wed. 10 Dec
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AUD 0.05

Multiples of: 10

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded2.2 uH5 %320 mA1 Ohms-- 40 C+ 105 C3075 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
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