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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Image  Information Image Stock Code(▲▼)Description
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Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
AISC-0805-R82G-T


RF Inductors - SMD FIXED IND 820NH 180MA 2.3 OHM
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ABRACON 1940
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.3263

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Wirewound0805 (2012 METRIC)Unshielded820 nH2 %180 mA2.3 Ohms - 40 C+ 125 C23250 MHzStandard2.29 mm1.73 mm1.55 mm Ceramic AISC - 0805Reel , Cut Tape
B82422A1183K100


RF Inductors - SMD SMT-INDUCTOR 1210 18 UH 10%, AEC-Q200
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TDK 1940
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.3736

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Wirewound1210 (3225 METRIC)Unshielded18 uH10 %155 mA2 Ohms-- 55 C+ 145 C2717 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
5-1624113-7


3650 0805 0.33uH 5% 2K R
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TE Connectivity 1940
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AUD 0.3965

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4-1624112-3


3650 0402 13nH 5% 2K RL
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TE Connectivity 1940
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AUD 0.4439

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4-1624112-7


INDUCTOR, 20NH, 3.5GHZ, 0402, WIREWOUND
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TE Connectivity 1940
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AUD 0.4439

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   20 nH                 
1-1624112-4


3650 0402 2.0nH 5% 2K RL
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TE Connectivity 1940
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between Mon. 24 Nov to Fri. 28 Nov
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AUD 0.4457

Multiples of: 2000

                     
IMC1812ESR33K


RF Inductors - SMD 33uh 10%
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Vishay 1940
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AUD 0.5137

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Molded1812 (4532 METRIC) 330 nH  820 mOhms     Standard      IMCReel , Cut Tape
ISC1210ER3R9K


RF Inductors - SMD 3.9uh 10%
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Vishay 1940
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AUD 0.5395

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Molded1210 (3225 METRIC) 3.9 uH10 %250 mA1.2 Ohms - 55 C+ 125 C3058 MHzStandard      ISCReel , Cut Tape
IMC1210ERR39K


RF Inductors - SMD 39uh 10%
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Vishay 1940
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AUD 0.6133

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Molded1210 (3225 METRIC) 390 nH10 %450 mA450 mOhms - 55 C+ 125 C30250 MHzStandard      IMCReel , Cut Tape
IMC1210ER2R7J


RF Inductors - SMD 2.7uh 5%
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Vishay 1940
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between Fri. 28 Nov to Tue. 02 Dec
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AUD 0.6211

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 1210 (3225 METRIC)Unshielded2.7 uH5 %390 mA1.1 Ohms    290 MHz-3.2 mm2.49 mm     Reel
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