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
  
                         
B82422A1122K100


RF Inductors - SMD SMT-INDUCTOR 1210 1.2UH 10%, AEC-Q200
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TDK 5442
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AUD 0.3121
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded1.2 uH10 %370 mA370 mOhms-- 55 C+ 145 C20300 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
LQG15HS33NJ02D


RF Inductors - SMD 33 NH 5%
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Murata 5432
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AUD 0.0086
Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded33 nH5 %350 mA580 mOhms-- 55 C+ 125 C81.6 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
MCQ1V1608-2R2-R


RF Inductors - SMD Multi H Q, IND2.2uH Q25 50mA 2PADS SMT
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Eaton 5432
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AUD 0.022
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Multilayer0603 (1608 METRIC)Unshielded2.2 uH10 %25 mA800 mOhms-- 40 C+ 85 C2550 MHzStandard1.6 mm0.8 mm0.8 mm-  MCQ1VReel , Cut Tape
B82432C1105K


RF Inductors - SMD SMT-INDUCTOR 1812 1000UH 10%
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TDK 5431
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AUD 0.6078
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Wirewound1812 (4532 METRIC)Unshielded1 mH10 %55 mA32 Ohms-- 55 C+ 150 C302.8 MHzStandard4.5 mm3.2 mm3.2 mm-FerriteAEC - Q200B82432CReel , Cut Tape
B82422T1103K


RF Inductors - SMD 10uH 150mA 10% 3.2x2.5mm SMD
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TDK 5420
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AUD 0.2802
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Wirewound1210 (3225 METRIC)Unshielded10 uH10 %150 mA2.1 Ohms-- 55 C+ 125 C2730 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422TReel , Cut Tape
LQW15AN4N0B80D


RF Inductors - SMD
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Murata 5403
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AUD 0.0546
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded4 nH0.1 nH1.95 A30 mOhms-- 55 C+ 125 C3010 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
MLF2012A1R5JT000


RF Inductors - SMD 2mm x 1.25mm x 0.85mm, -55 to +125 degC, 80mA, 1.5?H, 400mohm
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TDK 5385
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AUD 0.1133
Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded1.5 uH5 %80 mA400 mOhms-- 55 C+ 125 C45140 MHzStandard2 mm1.25 mm0.85 mm-Ferrite MLFReel , Cut Tape
MLG1005S1N1BTD25


RF Inductors - SMD IND 0402 1.1nH StdQ AEC Q200 RF IND
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TDK 5383
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AUD 0.0142
Multiples of: 50

Multilayer0402 (1005 METRIC)Unshielded1.1 nH0.1 nH1 A100 mOhms-- 55 C+ 125 C719.3 GHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
LQP02TN4N2B02D


RF Inductors - SMD
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Murata 5383
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AUD 0.0203
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Thin Film01005 (0402 METRIC)Unshielded4.2 nH0.1 nH180 mA1.3 Ohms - 55 C+ 125 C87 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
LQW15AN11NJ00D


RF Inductors - SMD 11 NH
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Murata 2657
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AUD 0.0367
Multiples of: 20

Wirewound0402 (1005 METRIC)Unshielded11 nH5 %500 mA140 mOhms-- 55 C+ 125 C305.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
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