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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(Ex. GST)(▲▼)		Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
IMC0805ERR56J01


RF Inductors - SMD .56uh 5%
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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.

Vishay 1913
Ships to you
between Thu. 23 Jul to Mon. 27 Jul Calender.png

AUD 0.188
Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded560 nH  1.1 Ohms - 40 C+ 125 C 340 MHzStandard2 mm1.25 mm1.2 mm Ferrite IMCReel , Cut Tape
CIGT201206UM1R0MNE


RF Inductors - SMD CIGT,Thin Film,0805,1.0uH,0.6?,7 embossed,-20 20%
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SAMSUNG 0
6 to 16 Weeks Calender.png

AUD 0.1855
Multiples of: 60000

Thin Film  1 uH20 %              CIGTReel , Cut Tape
IWC0402D33NR-3G


RF Inductors - SMD 0402 33nH 2% 400mA
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Laird Performance Materials 0
6 to 16 Weeks Calender.png

AUD 0.1855
Multiples of: 20000

Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded33 nH2 %400 mA450 mOhms-- 40 C+ 125 C242.35 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
L0201R68AHSTR


RF Inductors - SMD 0.68nH
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Kyocera AVX 0
6 to 16 Weeks Calender.png

AUD 0.1913
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded680 pH0.05 nH500 mA200 mOhms-- 55 C+ 125 C830 GHzStandard0.6 mm0.325 mm0.225 mm-  Accu - LReel , Cut Tape
LQW15AW82NG80D


RF Inductors - SMD Fixed IND 82nH 370mA NONAUTO
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Murata 0
6 to 16 Weeks Calender.png

AUD 0.181
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded82 nH2 %370 mA870 mOhms-- 55 C+ 125 C331.7 GHzStandard1.02 mm0.61 mm0.61 mm-  LQWReel , Cut Tape
NLV25T-R56J-EFD


RF Inductors - SMD 560nH 750mohms 325mA Wound Fer AEC-Q200
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TDK 0
6 to 16 Weeks Calender.png

AUD 0.1786
Multiples of: 1

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded560 nH5 %325 mA750 mOhms-- 40 C+ 105 C30325 MHzStandard2.5 mm2 mm1.8 mm-FerriteAEC - Q200NLV25 - EFDReel , Cut Tape
LQW2BAS33NG0CL


RF Inductors - SMD
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Murata 0
6 to 16 Weeks Calender.png

AUD 0.179
Multiples of: 2000

   33 nH2 %                
IWC0402A68NR-3G


RF Inductors - SMD 0402 68nH 2% 100mA
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Laird Performance Materials 0
6 to 16 Weeks Calender.png

AUD 0.1872
Multiples of: 20000

Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded68 nH2 %100 mA1.12 Ohms-- 40 C+ 125 C221.62 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
IWC0402A82NR-3G


RF Inductors - SMD 0402 82nH 2% 50mA
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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.

Laird Performance Materials 0
6 to 16 Weeks Calender.png

AUD 0.1872
Multiples of: 20000

Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded82 nH2 %50 mA1.55 Ohms-- 40 C+ 125 C201.23 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
IWC0402B39NR-3G


RF Inductors - SMD 0402 39nH 2% 200mA
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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.

Laird Performance Materials 0
6 to 16 Weeks Calender.png

AUD 0.1872
Multiples of: 20000

Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded39 nH2 %200 mA550 mOhms-- 40 C+ 125 C252.1 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
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