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
  
                         
NLV25T-5R6J-EF


RF Inductors - SMD 5.6uH 2.5ohms 170mA Wound Ferrite
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TDK 2434
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between Mon. 08 Dec to Thu. 11 Dec
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AUD 0.0515

Multiples of: 10

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded5.6 uH5 %170 mA2.5 Ohms-- 40 C+ 105 C2542 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
MLF2012A3R3M


RF Inductors - SMD 3.3uH
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TDK 2289
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.0908

Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded3.3 uH20 %50 mA600 mOhms-- 55 C+ 125 C4590 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
MHQ1005P51NJT000


RF Inductors - SMD IND 0402 51nH S-HQ SMD RF IND
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TDK 2281
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1027

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded51 nH5 %190 mA1.8 Ohms-- 55 C+ 125 C221.8 GHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
LQW15CN34NJ10D


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 2269
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between Mon. 08 Dec to Thu. 11 Dec
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AUD 0.1344

Multiples of: 5

Wirewound0402 (1005 METRIC)Unshielded34 nH5 %1.8 A36 mOhms - 55 C+ 125 C 2.5 GHzStandard1 mm0.6 mm0.5 mm   LQWReel , Cut Tape
LQW18AN10NJ10D


RF Inductors - SMD 10 NH 5%
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Murata 2269
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between Mon. 08 Dec to Thu. 11 Dec
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AUD 0.0611

Multiples of: 10

Wirewound0603 (1608 METRIC)Unshielded10 nH5 %800 mA58 mOhms-- 55 C+ 125 C387 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
MCQ1V3216-R150-R


RF Inductors - SMD Multi H Q,IND 150nH Q25 250mA 2PADS SMT
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Eaton 2261
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.0495

Multiples of: 1

Multilayer1206 (3216 METRIC)Unshielded150 nH10 %250 mA250 mOhms-- 40 C+ 85 C25200 MHzStandard3.2 mm1.6 mm0.9 mm-  MCQ1VReel , Cut Tape
ILSB1206ER3R9K


RF Inductors - SMD 3.9uH 10%
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Vishay 2257
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1413

Multiples of: 1

Established Reliability1206 (3216 METRIC)Shielded3.9 uH10 %50 mA800 mOhms-- 55 C+ 125 C4544 MHzStandard3.2 mm1.6 mm1.1 mm-  ILSB - 1206Reel , Cut Tape
MLF2012DR82KTD25


RF Inductors - SMD 820nH 650mohms 150mA +/-10% Fer AEC-Q200
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TDK 2245
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.1438

Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded820 nH10 %150 mA650 mOhms-- 55 C+ 125 C25170 MHzStandard2 mm1.25 mm1.25 mm-FerriteAEC - Q200MLFReel , Cut Tape
MLF2012E100KTD25


RF Inductors - SMD 10uH 800mohms 15mA +/-10% Fer AEC-Q200
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TDK 2158
Ships to you
between Mon. 08 Dec to Thu. 11 Dec
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AUD 0.095

Multiples of: 5

Multilayer0805 (2012 METRIC)Shielded10 uH10 %15 mA800 mOhms-- 55 C+ 125 C5050 MHzStandard2 mm1.25 mm1.25 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQW15AN1N8C0ZD


RF Inductors - SMD 1.8 NH +/-0.2NH
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Murata 0
6 to 16 Weeks Calender.png

AUD 0.0087

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded1.8 nH0.2 nH460 mA160 mOhms-- 55 C+ 125 C1016 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
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