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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Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
AL023538NGTS


RF Inductors - SMD 538 NH 2%
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Kyocera AVX 0
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AUD 1.1197

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                 Air  Reel , Cut Tape
0402DC-16NXJRW


RF Inductors - SMD 1005 16nH Unshld 5% 1.2A 120mOhms
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Coilcraft 0
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AUD 1.1207

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded16 nH5 %1.2 A120 mOhms-- 40 C+ 125 C1025.95 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
0201DS-7N0XJEW


RF Inductors - SMD 0603 7nH Unshld 5% 390mA 210mOhms
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Coilcraft 0
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AUD 1.1261

Multiples of: 1

Wirewound0201 (0603 METRIC)Unshielded7 nH5 %390 mA210 mOhms-- 40 C+ 125 C396.7 GHzStandard0.58 mm0.46 mm0.45 mm-Ceramic 0201DSReel , Cut Tape
0201DS-9N6XJEW


RF Inductors - SMD 0603 9.6nH Unshld 5% 280mA 400mOhms
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Coilcraft 0
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AUD 1.1261

Multiples of: 1

Wirewound0201 (0603 METRIC)Unshielded9.6 nH5 %280 mA400 mOhms - 40 C+ 125 C386.2 GHzStandard0.58 mm0.46 mm0.45 mm Ceramic 0201DSReel , Cut Tape
0201DS-13NXJEW


RF Inductors - SMD 0603 13nH Unshld 5% 270mA 440mOhms
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Coilcraft 0
6 to 16 Weeks Calender.png

AUD 1.1261

Multiples of: 1

Wirewound0201 (0603 METRIC)Unshielded13 nH5 %270 mA440 mOhms - 40 C+ 125 C386.7 GHzStandard0.58 mm0.46 mm0.45 mm Ceramic 0201DSReel , Cut Tape
0201DS-3N6XJEW


RF Inductors - SMD 0603 3.6nH Unshld 5% 550mA 105mOhms
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Coilcraft 0
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AUD 1.1261

Multiples of: 1

Wirewound0201 (0603 METRIC)Unshielded3.6 nH5 %550 mA105 mOhms - 40 C+ 125 C4012.5 GHzStandard0.58 mm0.46 mm0.45 mm Ceramic 0201DSReel , Cut Tape
0201DS-3N8XJEW


RF Inductors - SMD 0603 3.8nH Unshld 5% 420mA 180mOhms
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Coilcraft 0
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AUD 1.1261

Multiples of: 1

Wirewound0201 (0603 METRIC)Unshielded3.8 nH5 %420 mA180 mOhms - 40 C+ 125 C3810.2 GHzStandard0.58 mm0.46 mm0.45 mm Ceramic 0201DSReel , Cut Tape
0201DS-9N4XJEW


RF Inductors - SMD 0603 9.4nH Unshld 5% 280mA 400mOhms
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Coilcraft 0
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AUD 1.1261

Multiples of: 1

Wirewound0201 (0603 METRIC)Unshielded9.4 nH5 %280 mA400 mOhms - 40 C+ 125 C366.4 GHzStandard0.58 mm0.46 mm0.45 mm Ceramic 0201DSReel , Cut Tape
0807SQ-14NGLC


RF Inductors - SMD 13.7nH Unshld 2% 2.7A 8mOhms
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AUD 1.1311

Multiples of: 1

Wirewound1.829 mm x 1.524 mm x 1.93 mmUnshielded13.7 nH2 %2.7 A8 mOhms-- 40 C+ 125 C1004.3 GHzStandard1.93 mm1.829 mm1.524 mm-Air 080xSQReel , Cut Tape
1008CS-681XGRC


RF Inductors - SMD RF chip inductor
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AUD 1.1332

Multiples of: 1

   680 nH2 %                
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