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
  
                         
LQW18AN17NG8ZD


RF Inductors - SMD
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Murata 3880
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AUD 0.1477
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded17 nH2 %1.4 A75 mOhms-- 55 C+ 125 C404.6 GHzStandard1.65 mm0.99 mm0.9 mm--AEC - Q200LQWReel , Cut Tape
AISC-Q0603-33NG-T


RF Inductors - SMD IND 33nH 0.6A 220m?
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Abracon 3880
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AUD 0.1486
Multiples of: 1

Ceramic Wirewound RF Inductor0603 (1812 METRIC)Unshielded33 nH2 %600 mA220 mOhms - 40 C+ 125 C402.3 GHzStandard1.8 mm1.12 mm1.02 mm   AISC - Q0603Reel , Cut Tape
AISC-1210HS-6R8K-T2


RF Inductors - SMD 6.8 UH 10%
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ABRACON 3880
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AUD 0.1488
Multiples of: 2000

Wirewound1210 (3225 METRIC)Unshielded6.8 uH10 %480 mA1.1 Ohms500 mA- 40 C+ 85 C1055 MHzStandard3.2 mm3.05 mm1.3 mm Ferrite AISC - 1210HSReel , Cut Tape
LQW18AN10NG1ZD


RF Inductors - SMD
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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.

Murata 3880
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AUD 0.1535
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Wirewound0603 (1608 METRIC)Unshielded10 nH2 %800 mA58 mOhms-- 55 C+ 125 C385 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
BWCM0016100856NG00


RF Inductors - SMD 0402 56nH
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Pulse 3880
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AUD 0.1615
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 1.6 mm x 1.02 mm x 0.82 mmUnshielded56 nH2 %360 mA350 mOhms360 mA- 55 C+ 125 C382.4 GHzStandard1.6 mm1.02 mm0.82 mm-Ceramic BWCMReel , Cut Tape
AISC-Q0402-23NG-T


RF Inductors - SMD IND 23nH 0.4A 300m?
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Abracon 3880
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AUD 0.1638
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded23 nH2 %400 mA300 mOhms - 40 C+ 125 C242.72 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
AISC-Q0402-6N8G-T


RF Inductors - SMD IND 6.8nH 0.68A 83m?
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Abracon 3880
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AUD 0.1638
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded6.8 nH2 %680 mA83 mOhms - 40 C+ 125 C204.8 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
AISC-Q0402-22NG-T


RF Inductors - SMD IND 22nH 0.4A 300m?
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Abracon 3880
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AUD 0.1638
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded22 nH2 %400 mA300 mOhms - 40 C+ 125 C252.8 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
AISC-Q0402-39NG-T


RF Inductors - SMD IND 39nH 0.2A 550m?
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Abracon 3880
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AUD 0.1638
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded39 nH2 %200 mA550 mOhms - 40 C+ 125 C252.1 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
AISC-Q0402-27NG-T


RF Inductors - SMD IND 27nH 0.4A 300m?
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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.

Abracon 3880
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AUD 0.1638
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded27 nH2 %400 mA300 mOhms - 40 C+ 125 C242.48 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
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