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
  
                         
MLG1005S68NJT000


RF Inductors - SMD IND 0402 68nH StdQ SMD RF IND
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TDK 6984
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AUD 0.0094
Multiples of: 10

Multilayer0402 (1005 METRIC)Unshielded68 nH5 %200 mA1.5 Ohms-- 55 C+ 125 C81.1 GHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , Cut Tape
NLV32T-180J-EFD


RF Inductors - SMD 18uH 3.3ohms 120mA Wound Fer AEC-Q200
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TDK 6962
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AUD 0.1614
Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded18 uH5 %120 mA3.3 Ohms-- 40 C+ 105 C3020 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
LQW15AN4N6C8ZD


RF Inductors - SMD
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Murata 6959
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AUD 0.1293
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Wirewound0402 (1005 METRIC)Unshielded4.6 nH0.2 nH1.45 A60 mOhms-- 55 C+ 125 C9.69.6 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
MLF1608DR33MTA00


RF Inductors - SMD 1.6mm x 0.8mm x 0.8mm, -55 to +125 degC, 100mA, 0.33?H, 750mohm
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TDK 6954
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AUD 0.0872
Multiples of: 1

Multilayer0603 (1608 METRIC)Shielded330 nH20 %100 mA750 mOhms-- 55 C+ 125 C15320 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
LQW15AN8N4G8ZD


RF Inductors - SMD
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Murata 6954
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AUD 0.1413
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded8.4 nH2 %1.5 A69 mOhms-- 55 C+ 125 C6.56.5 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQW18AS3N3G0ZD


RF Inductors - SMD 3.3 NH 2% NH
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Murata 6951
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AUD 0.1155
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded3.3 nH2 %700 mA45 mOhms-- 40 C+ 125 C355.9 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
MLF1608D68NMTD25


RF Inductors - SMD 68nH 300mohms 200mA +/-20% Fer AEC-Q200
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TDK 6949
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AUD 0.1252
Multiples of: 1

Multilayer0603 (1608 METRIC)Shielded68 nH20 %200 mA300 mOhms-- 55 C+ 125 C10700 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
MLF2012A1R5JTD25


RF Inductors - SMD 1.5uH 400mohms 80mA +/-5% Fer AEC-Q200
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TDK 6948
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AUD 0.1629
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Multilayer0805 (2012 METRIC)Shielded1.5 uH5 %80 mA400 mOhms-- 55 C+ 125 C45140 MHzStandard2 mm1.25 mm0.85 mm-FerriteAEC - Q200MLFReel , Cut Tape
CI160808-82NJ


RF Inductors - SMD 82nH 5% MultiLayer High Frequency
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Bourns 6945
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AUD 0.0513
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Multilayer0603 (1608 METRIC)Unshielded82 nH5 %300 mA1.5 Ohms-- 55 C+ 125 C10600 MHzStandard1.6 mm0.8 mm0.8 mm-Ceramic CI160808Reel , Cut Tape
MCQ1V1608-R047-R


RF Inductors - SMD Multi H Q, IND 47nH Q15 50mA 2PADS SMT
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Eaton 6940
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AUD 0.0202
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Multilayer0603 (1608 METRIC)Unshielded47 nH10 %50 mA200 mOhms-- 40 C+ 85 C15260 MHzStandard1.6 mm0.8 mm0.8 mm-  MCQ1VReel , Cut Tape
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