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
  
                         
1210ASM-R33J-01


RF Inductors - SMD 330nH 5% tol Non-Mag Chip IND
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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.

Fastron 776
Ships to you
between Fri. 17 Jul to Thu. 23 Jul Calender.png

AUD 0.5808
Multiples of: 1

Wirewound3.8 mm x 3 mm x 2.4 mmUnshielded330 nH5 %680 mA490 mOhms - 40 C+ 150 C45500 MHzStandard3.8 mm3 mm2.4 mm CeramicAEC - Q2001210ASMReel
IWC0805DR18R-3G


RF Inductors - SMD 0805 180nH 2% 400mA
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Laird Performance Materials 0
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AUD 0.2299
Multiples of: 10000

Wirewound2.35 mm x 1.73 mm x 1.52 mmUnshielded180 nH2 %400 mA640 mOhms-- 40 C+ 125 C50870 MHzStandard2.35 mm1.73 mm1.52 mm-Ceramic IWC0805Reel , Cut Tape
CW100505-56NJ


RF Inductors - SMD 56.0 nH 5% 200 MHz 0.97ohms
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Bourns 0
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AUD 0.2217
Multiples of: 10000

 0402 (1005 METRIC)Unshielded56 nH5 %200 mA970 mOhms - 55 C+ 125 C221.76 GHzStandard1 mm0.55 mm0.5 mm Ceramic CW100505Reel
AISC-1210-82NJ-T


RF Inductors - SMD FIXED IND 82NH 900MA 200 MOHM
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ABRACON 0
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AUD 0.2243
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Wirewound1210 (3225 METRIC)Unshielded82 nH5 %900 mA200 mOhms - 40 C+ 125 C551 GHzStandard3.65 mm2.95 mm2.7 mm Ceramic AISC - 1210Reel , Cut Tape
AL01622N0JTS


RF Inductors - SMD 22nH 5% AIR CORE
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Kyocera AVX 0
6 to 16 Weeks Calender.png

AUD 0.2253
Multiples of: 1000

Wirewound3.81 mm x 4.2 mm x 4.83 mmUnshielded22 nH5 %3 A4.2 mOhms-- 40 C+ 125 C1003.2 GHzStandard4.83 mm3.81 mm4.2 mm-Air ALReel , Cut Tape
0603AS-R20G-01


RF Inductors - SMD 200nH 100 MHz 2% Tol
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Fastron 0
6 to 16 Weeks Calender.png

AUD 0.2293
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded200 nH2 %200 mA1.55 Ohms-- 40 C+ 150 C301.1 GHzStandard1.52 mm0.76 mm1 mm-CeramicAEC - Q2000603ASReel , Cut Tape
0402WL1R0JT


RF Inductors - SMD INDUCTOR -RESALE
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Kyocera AVX 0
6 to 16 Weeks Calender.png

AUD 0.2308
Multiples of: 1

                   WLReel , Cut Tape
AIAC-2712C-17N5J-T


RF Inductors - SMD FIXED IND 17.5NH 3.5A 4.5 MOHM
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ABRACON 0
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AUD 0.231
Multiples of: 2000

SMT Air Coil Inductor6 mm x 2.5 mm x 2.6 mmUnshielded17.5 nH5 %3.5 A4.5 mOhms - 40 C+ 125 C1002.2 GHzStandard6 mm2.5 mm2.6 mm Air AIAC - 2712CReel , Cut Tape
WCL3225-221-R


INDUCTOR, 220UH, 2.6MHZ, 1210
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Eaton 0
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AUD 0.2321
Multiples of: 1

   220 uH         3.5 mm2.9 mm2.25 mm   WCLReel , Cut Tape
IWC1008J27NR-3G


RF Inductors - SMD 1008 27nH 2% 1000mA
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Laird Performance Materials 0
6 to 16 Weeks Calender.png

AUD 0.243
Multiples of: 10000

Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded27 nH2 %1 A130 mOhms-- 40 C+ 125 C551.6 GHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
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