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
  
                         
B82422T1222K


RF Inductors - SMD 2.2uH 320mA 10% 3.2x2.5mm SMD
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TDK 3455
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AUD 0.2568
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded2.2 uH10 %320 mA800 mOhms-- 55 C+ 125 C30100 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422TReel , Cut Tape
AISC-0402-9N0J-T


RF Inductors - SMD FIXED IND 9NH 680MA 100 MOHM SMD
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ABRACON 3453
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AUD 0.0296
Multiples of: 5

Smd Ceramic Wire - Wound Chip Inductors0402 (1005 METRIC)Unshielded9 nH5 %680 mA100 mOhms - 40 C+ 125 C254160 MHz     Ceramic Aisc - 0402Reel
AISC-Q0805-R51G-T


RF Inductors - SMD IND 510nH 0.24A 1900m?
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Abracon 3437
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AUD 0.179
Multiples of: 1

Ceramic Wirewound RF Inductor0805 (2317 METRIC)Unshielded510 nH2 %240 mA1.9 Ohms - 40 C+ 125 C23365 MHzStandard2.29 mm1.73 mm1.52 mm   AISC - Q0805Reel , Cut Tape
MLG1005SR22HT000


RF Inductors - SMD IND 0402 220nH StdQ SMD RF IND
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TDK 3424
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AUD 0.008
Multiples of: 10

Multilayer0402 (1005 METRIC)Unshielded220 nH3 %100 mA4.2 Ohms-- 55 C+ 125 C8500 MHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , Cut Tape
AISC-Q0402HQ-2N2C-T


RF Inductors - SMD IND 2.2nH 2.1A 38m?
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Abracon 3422
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AUD 0.197
Multiples of: 1

Wirewound0402 (1208 METRIC)Unshielded2.2 nH0.2 nH2.1 A38 mOhms - 40 C+ 125 C8615.1 GHzStandard1.27 mm0.76 mm0.61 mm Ceramic AISC - Q0402HQReel , Cut Tape
CW252016-R33J


Inductor RF Wirewound 0.33uH 5% 25.2MHz 45Q-Factor Ceramic 0.45A 1.05Ohm DCR 1008 T/R
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Bourns 3411
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AUD 0.1776
Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded330 nH5 %500 mA900 mOhms-- 40 C+ 125 C45570 MHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
MLF1608A2R2JTD25


RF Inductors - SMD 2.2uH 1.0ohms 30mA +/-5% Fer AEC-Q200
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TDK 3298
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AUD 0.1005
Multiples of: 5

Multilayer0603 (1608 METRIC)Shielded2.2 uH5 %30 mA1 Ohms-- 55 C+ 125 C35120 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
B82422-A1102-J100


RF Inductors - SMD SMT-INDUCTOR 1210 1 UH 5%, AEC-Q200
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TDK 3290
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AUD 0.3
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded1 uH5 %380 mA340 mOhms-- 55 C+ 145 C20320 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
AISC-Q0402-12NG-T


RF Inductors - SMD IND 12nH 0.64A 120m?
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Abracon 2975
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AUD 0.1494
Multiples of: 1

Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded12 nH2 %640 mA120 mOhms - 40 C+ 125 C243.6 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
MLG1005S2N4STD25


RF Inductors - SMD IND 0402 2.4nH StdQ AEC Q200 RF IND
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TDK 873
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AUD 0.0163
Multiples of: 50

Multilayer0402 (1005 METRIC)Unshielded2.4 nH0.3 nH800 mA150 mOhms-- 55 C+ 125 C78.2 GHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
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