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
  
                         
5598 821 34 00


RF Inductors - SMD RF Chip Inductor SMD 820nH 0805 5% Tol
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Sumida 0
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AUD 0.2978

Multiples of: 9000

 0805 (2012 METRIC)Unshielded820 nH5 %75 mA5 Ohms - 55 C+ 125 C35510 MHzStandard2.2 mm1.4 mm1.42 mm   5508Reel
4-1624113-6


3650 0805 0.10uH 5% 2K R
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TE Connectivity 0
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AUD 0.2981

Multiples of: 2000

                     
0402AS-068J-08


RF Inductors - SMD 68nH 250MHz 5% Tol
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Fastron 0
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AUD 0.2984

Multiples of: 1

Wirewound0402 (1005 METRIC) 68 nH5 %100 mA970 mOhms   251.62 GHzStandard1.2 mm0.65 mm0.7 mm  AEC - Q2000402ASReel
CMH322522-8R2KL


RF Inductors - SMD 8.2uH 10% 7.96MHz
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Bourns 0
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AUD 0.2988

Multiples of: 1

Wirewound1210 (3225 METRIC)Shielded8.2 uH10 %170 mA2 Ohms-- 55 C+ 125 C3030 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite  Reel , Cut Tape
LCWC0603G22NGTAR


RF Inductors - SMD 22nH 0603 2%
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Kyocera AVX 0
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AUD 0.3136

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded22 nH2 %700 mA190 mOhms - 40 C+ 125 C383 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic LCWCReel , Cut Tape
KL732ATTE22NJ


RF Inductors - SMD 22 NH 5% (R)
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KOA Speer 0
6 to 16 Weeks Calender.png

AUD 0.3009

Multiples of: 1

Thin Film0805 (2012 METRIC)Unshielded22 nH5 %150 mA5 Ohms-- 40 C+ 125 C2010 GHzStandard2 mm1.25 mm0.5 mm- AEC - Q200KL73Reel , Cut Tape
LQG15WH3N3S02D


RF Inductors - SMD
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Murata 0
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AUD 0.3023

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded3.3 nH0.3 nH900 mA80 mOhms-- 55 C+ 125 C236 GHzStandard1 mm0.6 mm0.5 mm AirAEC - Q200LQGReel , Cut Tape
AL12A12N5JTR


RF Inductors - SMD 12.5nH 5% Air Core
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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.

Kyocera AVX 0
6 to 16 Weeks Calender.png

AUD 0.3207

Multiples of: 1

Wirewound3.05 mm x 3.18 mm x 3.68 mmUnshielded12.5 nH5 %4 A3.4 mOhms-- 40 C+ 125 C1373.3 GHzStandard3.68 mm3.05 mm3.18 mm-Air ALReel , Cut Tape
KL732ATTE47NJ


RF Inductors - SMD 47 NH 5% (R)
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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.

KOA Speer 0
6 to 16 Weeks Calender.png

AUD 0.3067

Multiples of: 1

Thin Film0805 (2012 METRIC)Unshielded47 nH5 % 2.5 Ohms - 40 C+ 125 C 600 MHzStandard2 mm1.25 mm   AEC - Q200KL73Reel , Cut Tape
LQH2HNH1R0M03L


RF Inductors - SMD 1uH 480mA 20% PWRTRN AEC-Q200
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Murata 0
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AUD 0.3075

Multiples of: 3000

Wirewound2.5 mm x 2 mm x 0.5 mmUnshielded1 uH20 % 115 mOhms - 40 C+ 125 C 150 MHzStandard2.5 mm2 mm0.9 mm  AEC - Q200LQH2HNH_03Reel , Cut Tape
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