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
  
                         
NLV32T-2R7J-EF


RF Inductors - SMD 2.7uH 1.1ohms 290mA Wound Ferrite
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TDK 3579
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AUD 0.0476
Multiples of: 10

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded2.7 uH5 %290 mA1.1 Ohms-- 40 C+ 105 C3070 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
MLF2012DR82JTD25


RF Inductors - SMD 820nH 650mohms 150mA +/-5% Fer AEC-Q200
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TDK 3102
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AUD 0.1517
Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded820 nH5 %150 mA650 mOhms-- 55 C+ 125 C25170 MHzStandard2 mm1.25 mm1.25 mm-FerriteAEC - Q200MLFReel , Cut Tape
AISC-0402-3N6J-T


RF Inductors - SMD FIXED IND 3.6NH 840MA 66 MOHM
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ABRACON 3099
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AUD 0.0286
Multiples of: 5

Smd Ceramic Wire - Wound Chip Inductors0402 (1005 METRIC)Unshielded3.6 nH5 %840 mA66 mOhms - 40 C+ 125 C206800 MHz 1.19 mm0.64 mm0.66 mm Ceramic Aisc - 0402Reel
MCLA3216V1-1R2-R


RF Inductors - SMD MCLA Auto Chip IND 3216 1.2uH 2 Pads
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Eaton 3095
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AUD 0.0897
Multiples of: 1

Multilayer1206 (3216 METRIC)Unshielded1.2 uH10 %100 mA400 mOhms-- 40 C+ 125 C3565 MHzStandard3.2 mm1.6 mm0.9 mm-  MCLAReel , Cut Tape
PE-1008CD470GTT


RF Inductors - SMD SMD IND
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Pulse 3088
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AUD 0.3124
Multiples of: 1

Multilayer1008 (2520 METRIC)Unshielded47 nH2 %1 A80 mOhms - 40 C+ 125 C651.2 GHzStandard2.92 mm2.79 mm2.29 mm-Ceramic CDReel , Cut Tape
AIMC-0805-82NJ-T


RF Inductors - SMD 82 UH +/-5%
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ABRACON 3079
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AUD 0.1982
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Multilayer0805 (2012 METRIC)Shielded82 nH5 %300 mA900 mOhms - 55 C+ 125 C18600 MHzStandard2 mm1.25 mm0.85 mm Ceramic AIMC - 0805Reel , Cut Tape
LQW18AN36NJ80D


RF Inductors - SMD
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Murata 3074
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AUD 0.1252
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded36 nH5 %910 mA200 mOhms-- 55 C+ 125 C373 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
AISC-1008-5R6J-T


RF Inductors - SMD FIXED IND 5.6UH 240MA 5.7 OHM
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ABRACON 3070
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AUD 0.0326
Multiples of: 5

Wirewound1008 (2520 METRIC)Unshielded5.6 uH5 %240 mA5.7 Ohms - 40 C+ 125 C2040 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
CIGT201608EHR47MNE


RF Inductors - SMD CIGT,Thin Film,0806,0.47uH,0.8?,7 embossed,-20 20%
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SAMSUNG 3070
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AUD 0.1281
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Thin Film Shielded470 nH20 %4.3 A27 mOhms - 40 C+ 125 C--Standard2 mm1.6 mm0.8 mm-Metal Composite CIGTReel , Cut Tape
CW201212-12NJ


RF Inductors - SMD 12nH 5% HIGH Q
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Bourns 3070
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AUD 0.2052
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Wirewound0805 (2012 METRIC)Unshielded12 nH5 %600 mA80 mOhms-- 40 C+ 125 C604.1 GHzStandard2.1 mm1.5 mm1.3 mm-Ceramic CW201212Reel , Cut Tape
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