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
  
                         
AISC-0805HQ-10NJ-T


RF Inductors - SMD FIXED IND 10NH 1.6A 60 MOHM 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.

ABRACON 0
6 to 16 Weeks Calender.png

AUD 0.3448

Multiples of: 1

Wirewound0805 (2317 METRIC)Unshielded10 nH5 %1.6 A60 mOhms - 40 C+ 125 C803 GHzStandard2.29 mm1.73 mm1.52 mm Ceramic AISC - 0805HQReel , Cut Tape
AISC-0805HQ-18NJ-T


RF Inductors - SMD FIXED IND 18NH 1.4A 60 MOHM SMD
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ABRACON 0
6 to 16 Weeks Calender.png

AUD 0.3448

Multiples of: 1

Wirewound0805 (2317 METRIC)Unshielded18 nH5 %1.4 A60 mOhms - 40 C+ 125 C752.55 GHzStandard2.29 mm1.73 mm1.52 mm Ceramic AISC - 0805HQReel , Cut Tape
L06032R7CGWTR


RF Inductors - SMD 2.7nH
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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
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AUD 0.3452

Multiples of: 3000

Thin Film0603 (1608 METRIC)Unshielded2.7 nH0.2 nH750 mA80 mOhms-- 55 C+ 125 C219 GHzStandard1.6 mm0.81 mm0.61 mm-  0603, 0805Reel , Cut Tape
0402AS-047J-08


RF Inductors - SMD 47nH 250MHz 5% Tol
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Fastron 0
6 to 16 Weeks Calender.png

AUD 0.346

Multiples of: 10

Wirewound0402 (1005 METRIC) 47 nH5 %150 mA830 mOhms   252.1 GHzStandard1.2 mm0.65 mm0.7 mm  AEC - Q2000402ASReel
5406 033 24 00


RF Inductors - SMD RF Chip Inductor SMD 3.3nH 0603 10% Tol
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Sumida 0
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AUD 0.3467

Multiples of: 12000

 0603 (1608 METRIC)Unshielded3.3 nH 800 mA40 mOhms - 55 C+ 125 C306 GHzStandard1.7 mm1.2 mm0.85 mm   5406Reel
1210AS-R22J-01


RF Inductors - SMD RF CHIP INDUCTORS
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Fastron 0
6 to 16 Weeks Calender.png

AUD 0.3723

Multiples of: 800

Wirewound1210 (3225 METRIC)Unshielded220 nH5 %790 mA350 mOhms-- 40 C+ 125 C50650 MHzStandard3.8 mm3 mm2.4 mm-CeramicAEC - Q2001210ASReel , Cut Tape
LQW15CN3R3M10D


RF Inductors - SMD 3.3 UH 20%
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Murata 0
6 to 16 Weeks Calender.png

AUD 0.352

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded3.3 uH20 %130 mA3.65 Ohms-- 55 C+ 125 C 80 MHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
0805F-1R0K-08


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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Fastron 0
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AUD 0.3554

Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded1 uH10 %250 mA500 mOhms - 40 C+ 150 C20350 MHzStandard2.3 mm1.6 mm1.6 mm FerriteAEC - Q2000805FReel
AIAC-1008C-82NK-T


RF Inductors - SMD FIXED IND 82NH 320MA 51.5 MOHM
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AUD 0.3556

Multiples of: 1

 1008 (2520 METRIC)Unshielded82 nH10 %320 mA51.5 Ohms - 40 C+ 125 C701000 MHz 2.2 mm1.9 mm2.2 mm   Aiac - 1008CReel
LQH2HNHR82K03L


RF Inductors - SMD 0.82uH 550mA 10% PWRTRN AEC-Q200
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Murata 0
6 to 16 Weeks Calender.png

AUD 0.3556

Multiples of: 1

Wirewound2.5 mm x 2 mm x 0.5 mmUnshielded820 nH10 % 90 mOhms - 40 C+ 125 C 180 MHzStandard2.5 mm2 mm0.9 mm  AEC - Q200LQH2HNH_03Reel , Cut Tape
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