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
  
                         
NLCV25T-2R2M-EFRD


RF Inductors - SMD 2.2uH 0.27ohms 730mA 2.5x2.0mm AEC-Q200
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TDK 1673
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AUD 0.1153
Multiples of: 5

Wirewound  2.2 uH20 %730 mA324 mOhms - 40 C+ 125 C  Standard2.5 mm2 mm1.9 mm  AEC - Q200NLCV - EFRDReel , Cut Tape
IMC1008ERR39J


RF Inductors - SMD 390nH 5%
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Vishay 1672
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AUD 0.1958
Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded390 nH5 %470 mA1.06 Ohms-- 40 C+ 125 C45530 MHzStandard2.5 mm2 mm1.6 mm-Ceramic IMCReel , Cut Tape
LQW2UAS82NJ00L


RF Inductors - SMD 82 NH 5%
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Murata 1668
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AUD 0.1276
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Wirewound1008 (2520 METRIC)Unshielded82 nH5 %1 A220 mOhms-- 55 C+ 125 C601 GHzStandard2.62 mm2.45 mm1.83 mm-Air LQWReel , Cut Tape
AISC-1206-39NJ-T


RF Inductors - SMD FIXED IND 39NH 1A 120 MOHM SMD
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ABRACON 1668
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AUD 0.5327
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Ceramic Wirewound RF Inductor1206 (3216 METRIC)Unshielded39 nH5 %1 A120 mOhms - 40 C+ 125 C501.8 GHzStandard3.56 mm2.16 mm1.52 mm Ceramic AISC - 1206Reel , Cut Tape
MLF2012K390MT000


RF Inductors - SMD 2mm x 1.25mm x 1.25mm, -40 to +85 degC, 4mA, 39?H, 2.4ohm
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TDK 1666
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AUD 0.0755
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Multilayer0805 (2012 METRIC)Shielded39 uH20 %4 mA2.4 Ohms-- 55 C+ 125 C3523 MHzStandard2 mm1.25 mm1.25 mm Ferrite MLFReel , Cut Tape
LQG15HHR12G02D


RF Inductors - SMD
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Murata 1664
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AUD 0.1361
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Multilayer0402 (1005 METRIC)Unshielded120 nH2 %200 mA1.3 Ohms - 55 C+ 125 C8600 MHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
IMC1008ER270J


RF Inductors - SMD 27uH 5%
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Vishay 1664
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AUD 0.21
Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded27 uH5 %95 mA6 Ohms-- 40 C+ 125 C1521 MHzStandard2.5 mm2 mm1.6 mm-Ferrite IMCReel , Cut Tape
LQW18AS33NJ0ZD


RF Inductors - SMD
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Murata 1663
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AUD 0.0082
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Wirewound0603 (1608 METRIC)Unshielded33 nH5 %600 mA220 mOhms-- 40 C+ 125 C402.3 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQG15HN1N1B02D


RF Inductors - SMD
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Murata 1663
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AUD 0.0525
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Multilayer0402 (1005 METRIC)Unshielded1.1 nH0.1 nH1 A80 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQP03HQ1N6B02D


1A 1.6nH 50mO 0201 Inductors (SMD) ROHS
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Murata 1561
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AUD 0.0497
Multiples of: 10

Thin Film0201 (0603 METRIC)Unshielded1.6 nH0.1 nH1 A50 mOhms-- 55 C+ 125 C2010 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
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