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
  
                         
0908SQ-22NJLC


RF Inductors - SMD 21.5nH Unshld 5% 4.4A 9mOhms
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AUD 1.0152

Multiples of: 1

  Unshielded21.5 nH5 %4.4 A9 mOhms - 40 C+ 125 C1303.7 GHzStandard2.79 mm2.29 mm2.03 mm Air 090xSQReel , Cut Tape
0402DC-6N8XJRW


RF Inductors - SMD 1005 6.8nH Unshld 5% 1.65A 63mOhms
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AUD 1.0185

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Wirewound0402 (1005 METRIC)Unshielded6.8 nH5 %1.65 A63 mOhms-- 40 C+ 125 C13810.15 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
0603DC-6N8XJRW


RF Inductors - SMD 0603 6.8nH 1330mA 5% DCR=.048OhmsAEC-Q200
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AUD 1.0303

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Wirewound0603 (1608 METRIC)Unshielded6.8 nH5 %2.58 A48 mOhms-- 40 C+ 125 C-5.1 GHzStandard1.7 mm0.99 mm0.89 mm-CeramicAEC - Q2000603DCReel , Cut Tape
0603DC-51NXJRW


RF Inductors - SMD 0603 51nH 570mA 5% DCR=.216OhmsAEC-Q200
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AUD 1.0303

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Wirewound0603 (1608 METRIC)Unshielded51 nH5 %1.17 A216 mOhms-- 40 C+ 125 C-1.95 GHzStandard1.7 mm0.99 mm0.89 mm-CeramicAEC - Q2000603DCReel , Cut Tape
0402DC-51NXJRW


RF Inductors - SMD 1005 51nH Unshld 5% 620mA 432mOhms
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AUD 1.0395

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded51 nH5 %620 mA432 mOhms-- 40 C+ 125 C543.35 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
1008HQ-68NXGLC


RF Inductors - SMD 1008 68nH Unshld 2% 1.1A 130mOhms
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AUD 1.0461

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded68 nH2 %1.1 A130 mOhms-- 40 C+ 125 C801.15 GHzStandard2.92 mm2.79 mm2.03 mm-Ceramic 1008HQReel , Cut Tape
0402DC-56NXJRW


RF Inductors - SMD 1005 56nH Unshld 5% 460mA 690mOhms
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AUD 1.0566

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded56 nH5 %460 mA690 mOhms-- 40 C+ 125 C543.21 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
0603CT-1N0XJRW


RF Inductors - SMD 0603 1nH Unshld 5% 1.6A 45mOhms
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AUD 1.0644

Multiples of: 1

Wirewound Unshielded1 nH5 %1.6 A45 mOhms-- 40 C+ 125 C-16 GHzStandard1.63 mm0.84 mm0.61 mm-Ceramic 0603CTReel , Cut Tape
0603CT-1N2XJRW


RF Inductors - SMD 0603 1.2nH Unshld 5% 1.1A 105mOhms
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AUD 1.0644

Multiples of: 1

   1.2 nH                 
0402DC-R12XJRW


RF Inductors - SMD 1005 120nH Unshld 5% 300mA 1.6 Ohms
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AUD 1.0655

Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded120 nH5 %300 mA1.6 Ohms-- 40 C+ 125 C462.2 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
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