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
  
                         
1210F-101K-01


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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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.

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AUD 0.4297

Multiples of: 1

Wirewound3.8 mm x 3 mm x 2.4 mmUnshielded100 uH10 %145 mA4.7 Ohms - 40 C+ 85 C224.5 MHzStandard3.8 mm3 mm2.4 mm FerriteAEC - Q2001210FReel
1210F-121K-01


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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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.

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6 to 16 Weeks Calender.png

AUD 0.4297

Multiples of: 1

Wirewound3.8 mm x 3 mm x 2.4 mmUnshielded120 uH10 %140 mA5.2 Ohms - 40 C+ 85 C304.2 MHzStandard3.8 mm3 mm2.4 mm FerriteAEC - Q2001210FReel
1210F-270K-01


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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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.

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6 to 16 Weeks Calender.png

AUD 0.4297

Multiples of: 1

Wirewound3.8 mm x 3 mm x 2.4 mmUnshielded27 uH10 %245 mA1.65 Ohms - 40 C+ 85 C269 MHzStandard3.8 mm3 mm2.4 mm FerriteAEC - Q2001210FReel
LQW03AW3N4C00D


RF Inductors - SMD
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Murata 0
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AUD 0.462

Multiples of: 10000

Wirewound0201 (0603 METRIC)Unshielded3.4 nH0.2 nH440 mA150 mOhms-- 55 C+ 125 C4311 GHzStandard0.53 mm0.4 mm0.4 mm-  LQWReel , Cut Tape
5508 220 34 00


RF Inductors - SMD RF Chip Inductor SMD 22nH 0805 5% Tol
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AUD 0.4368

Multiples of: 1

 0805 (2012 METRIC)Unshielded22 nH5 %600 mA90 mOhms - 55 C+ 125 C452.6 GHzStandard2.2 mm1.4 mm1.42 mm   5508Reel
5508 680 34 00


RF Inductors - SMD RF Chip Inductor SMD 68nH 0805 5% Tol
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AUD 0.4368

Multiples of: 1

 0805 (2012 METRIC)Unshielded68 nH5 %410 mA190 mOhms - 55 C+ 125 C451.55 GHzStandard2.2 mm1.4 mm1.42 mm   5508Reel
74479132


RF Inductors - SMD WE-MI SMT 1206 0.47 uH 10% IR = 200 mA RDC = 0.6 Ohms
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by Mon. 13 Jul
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AUD 0.4599

Multiples of: 1

 1206 (3216 METRIC) 470 nH10 %200 mA600 mOhms - 40 C+ 85 C25125 MHzStandard3.2 mm1.6 mm1.1 mm Ceramic WE - MIReel , Cut Tape
1206F-120J-01


RF Inductors - SMD Chip Inductor (Wire wound -open); 12H; Tol: 5%
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AUD 0.4415

Multiples of: 2000

Wirewound1206 (3216 METRIC)Unshielded12 uH5 % 4.3 Ohms     Standard    FerriteAEC - Q2001206FReel
1210F-681K-01


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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AUD 0.4457

Multiples of: 1

Wirewound3.8 mm x 3 mm x 2.4 mmUnshielded680 uH10 %65 mA25 Ohms - 40 C+ 85 C221.9 MHzStandard3.8 mm3 mm2.4 mm FerriteAEC - Q2001210FReel
AISC-1210-R27J-T


RF Inductors - SMD FIXED IND 270NH 630MA 400 MOHM
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AUD 0.4465

Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded270 nH5 %630 mA400 mOhms - 40 C+ 125 C40580 MHzStandard3.65 mm2.95 mm2.7 mm Ceramic AISC - 1210Reel , Cut Tape
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