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
  
                         
L0201R33AHSTR


RF Inductors - SMD 0.33nH
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Kyocera AVX 4501
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between Thu. 23 Jul to Mon. 27 Jul
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AUD 0.1586

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Thin Film0201 (0603 METRIC)Unshielded330 pH0.05 nH550 mA100 mOhms-- 55 C+ 125 C1335 GHzStandard0.6 mm0.325 mm0.225 mm-  Accu - LReel , Cut Tape
CW105550A-20NJ


RF Inductors - SMD 20nH 5 0.42A AEC-Q200
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Bourns 0
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AUD 0.1559

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Wirewound Unshielded20 nH5 %420 mA250 mOhms-- 40 C+ 125 C253 GHzStandard1 mm0.55 mm0.5 mm-CeramicAEC - Q200CW105550AReel
CW252016-68NJ


68 nH Unshielded Drum Core, Wirewound Inductor 600 mA 200mOhm Max 1008 (2520 Metric)
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Bourns 0
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AUD 0.1564

Multiples of: 2000

Wirewound1008 (2520 METRIC)Unshielded68 nH5 %600 mA150 mOhms-- 40 C+ 125 C601.3 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW252016Reel , Cut Tape
NLV25T-R12J-EFD


RF Inductors - SMD 120nH 300mohms 550mA Wound Fer AEC-Q200
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TDK 0
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AUD 0.1638

Multiples of: 1

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded120 nH5 %550 mA300 mOhms-- 40 C+ 105 C30700 MHzStandard2.5 mm2 mm1.8 mm-FerriteAEC - Q200NLV25 - EFDReel , Cut Tape
NLV25T-047J-EFD


RF Inductors - SMD 47nH 500mohms 360mA Wound Fer AEC-Q200
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TDK 0
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AUD 0.1638

Multiples of: 1

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded47 nH5 %360 mA500 mOhms-- 40 C+ 105 C201.2 GHzStandard2.5 mm2 mm1.8 mm-FerriteAEC - Q200NLV25 - EFDReel , Cut Tape
NLV25T-1R0J-EFD


RF Inductors - SMD 1.0uH 1.1ohms 245mA Wound Fer AEC-Q200
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TDK 0
6 to 16 Weeks Calender.png

AUD 0.1638

Multiples of: 1

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded1 uH5 %245 mA1.1 Ohms-- 40 C+ 105 C30245 MHzStandard2.5 mm2 mm1.8 mm-FerriteAEC - Q200NLV25 - EFDReel , Cut Tape
NLV32T-056J-EFD


RF Inductors - SMD 56nH 330mohms 450mA Wound Fer AEC-Q200
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TDK 0
6 to 16 Weeks Calender.png

AUD 0.1638

Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded56 nH5 %450 mA330 mOhms-- 40 C+ 105 C261.1 GHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
NLV32T-022J-EFD


RF Inductors - SMD 22nH 200mohms 450mA Wound Fer AEC-Q200
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TDK 0
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AUD 0.1638

Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded22 nH5 %450 mA200 mOhms-- 40 C+ 105 C231.7 GHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
NLV32T-027J-EFD


RF Inductors - SMD 27nH 220mohms 450mA Wound Fer AEC-Q200
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TDK 0
6 to 16 Weeks Calender.png

AUD 0.1589

Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded27 nH5 %450 mA220 mOhms-- 40 C+ 105 C231.5 GHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
LQG15WZ1N2B02D


RF Inductors - SMD
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Murata 0
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AUD 0.1568

Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded1.2 nH0.1 nH1.2 A30 mOhms-- 55 C+ 125 C-13 GHzStandard1 mm0.6 mm0.5 mm Air LQGReel
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