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
  
                         
LQW15AN14NG8ZD


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 5664
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.1535

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Wirewound0402 (1005 METRIC)Unshielded14 nH2 %1 A111 mOhms-- 55 C+ 125 C315.2 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQW18AS16NG00D


RF Inductors - SMD
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Murata 5658
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.0739

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Wirewound0603 (1608 METRIC)Unshielded16 nH2 %700 mA104 mOhms-- 40 C+ 125 C343.3 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
B82498F3560J000


RF Inductors - SMD 56nH 600mA 5% 2.3x1.7mm SMD
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TDK 5657
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AUD 0.3852

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Wirewound0805 (2012 METRIC)Unshielded56 nH5 %600 mA140 mOhms-- 55 C+ 125 C601.7 GHzStandard2 mm1.3 mm1.4 mm-Ceramic B82498FReel , Cut Tape
LQW15CAR80J00D


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 5656
Ships to you
between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.3017

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded800 nH5 %190 mA2.1 Ohms-- 40 C+ 125 C-770 MHzStandard1 mm0.5 mm0.5 mm-  LQWReel , Cut Tape
LQW15AN2N7C80D


RF Inductors - SMD
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Murata 5649
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.1373

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded2.7 nH0.2 nH1.5 A47 mOhms-- 55 C+ 125 C2814 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
MHQ0402PSA6N2HT000


RF Inductors - SMD 01005, 6.2nH +-3% S-HQ SMD RF IND
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TDK 5645
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.0293

Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded6.2 nH3 %200 mA1 Ohms-- 55 C+ 125 C106.89 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQW03AW11NJ00D


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 5643
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.4604

Multiples of: 1

Wirewound0201 (0603 METRIC)Unshielded11 nH5 %260 mA470 mOhms - 55 C+ 125 C377 GHzStandard0.53 mm0.4 mm0.4 mm   LQWReel , Cut Tape
KLZ2012NHR101LTD25


RF Inductors - SMD 100uH 2MHz 20% 2012 AEC-Q200
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TDK 5546
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.1435

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Multilayer0805 (2012 METRIC)Shielded100 uH20 %140 mA3.5 Ohms30 mA- 55 C+ 150 C--Flexible (Soft)2 mm1.25 mm1.25 mm-FerriteAEC - Q200KLZ - HRReel , Cut Tape
B82422A1153K100


RF Inductors - SMD 15uH 165mA 10% 1210 SMD, AEC-Q200
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TDK 4666
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.2663

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded15 uH10 %165 mA1.85 Ohms-- 55 C+ 145 C2720 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
B82498F1682J


RF Inductors - SMD SMT-INDUCTOR 0805 6.8 UH 5%
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TDK 2742
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between Tue. 14 Jul to Thu. 16 Jul
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AUD 0.4241

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Wirewound0805 (2012 METRIC)Unshielded6.8 uH5 %80 mA4.7 Ohms-- 55 C+ 125 C20140 MHzStandard2 mm1.3 mm1.4 mm-Ferrite B82498FReel , Cut Tape
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