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
  
                         
AISC-0805HQ-2N5J-T


RF Inductors - SMD RF wirewound chip inductors, 2.5nH, 5%, 80@1500MHz, 0.02 , 1600mA, 6GHz, 0805, Surface Mount, 2.29 x 1.73 x 1.52mm
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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 0.2343
Multiples of: 1

Wirewound0805 (2317 METRIC)Unshielded2.5 nH5 %1.6 A20 mOhms - 40 C+ 125 C806 GHzStandard2.29 mm1.73 mm1.52 mm Ceramic AISC - 0805HQReel , Cut Tape
AISC-0805HQ-6N8J-T


RF Inductors - SMD RF wirewound chip inductors, 6.8nH, 5%, 80@1000MHz, 0.035 , 1600mA, 4.4GHz, 0805, Surface Mount, 2.29 x 1.73 x 1.52mm
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AUD 0.2343
Multiples of: 1

Wirewound0805 (2317 METRIC)Unshielded6.8 nH5 %1.6 A35 mOhms - 40 C+ 125 C804.4 GHzStandard2.29 mm1.73 mm1.52 mm Ceramic AISC - 0805HQReel , Cut Tape
WCL3225-3R3-R


INDUCTOR, 3.3UH, 80MHZ, 1210
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Eaton 0
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AUD 0.2349
Multiples of: 1

   3.3 uH         3.5 mm2.9 mm2.25 mm   WCLReel , Cut Tape
CW100505-R10J


RF Inductors - SMD 100.0 nH 5% 150MHz 2.52ohms
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AUD 0.2358
Multiples of: 10000

 0402 (1005 METRIC)Unshielded100 nH5 %120 mA2.52 Ohms - 55 C+ 125 C201.3 GHzStandard1 mm0.55 mm0.5 mm Ceramic CW100505Reel
LQH44PN470MPRL


RF Inductors - SMD The factory is currently not accepting orders for this product.
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Murata 0
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AUD 0.2361
Multiples of: 5

   47 uH± 20 %                
0603AS-R27J-08


RF Inductors - SMD 270nH 100 MHz 5% Tol
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Fastron 0
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AUD 0.2373
Multiples of: 1000

Wirewound0603 (1608 METRIC)Unshielded270 nH5 %150 mA2.3 Ohms - 40 C+ 150 C30950 MHzStandard1.7 mm1.1 mm1 mm CeramicAEC - Q2000603ASReel
A03TJLC


RF Inductors - SMD 8nH Unshld 5% 4A 2.6mOhms AECQ2
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Coilcraft 0
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AUD 0.2414
Multiples of: 1

Wirewound4.45 mm x 3.15 mm x 3.94 mmUnshielded8 nH5 %4 A2.6 mOhms-- 40 C+ 125 C1405 GHzStandard3.94 mm4.45 mm3.15 mm-AirAEC - Q200A0XTReel , Cut Tape
CW160808-4N7J


RF Inductors - SMD 4.7nH 5%
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Bourns 0
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AUD 0.2416
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded4.7 nH5 %700 mA100 mOhms-- 40 C+ 125 C165.8 GHzStandard1.65 mm1.05 mm1 mm-Ceramic  Reel , Cut Tape
5-1624113-7


3650 0805 0.33uH 5% 2K R
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TE Connectivity 0
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AUD 0.2417
Multiples of: 2000

                     
IWC1008J39NR-3G


RF Inductors - SMD 1008 39nH 2% 1000mA
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Laird Performance Materials 0
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AUD 0.2528
Multiples of: 10000

Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded39 nH2 %1 A150 mOhms-- 40 C+ 125 C601.5 GHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
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