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
  
                         
MLF2012C101M


RF Inductors - SMD 100uH
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TDK 1940
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AUD 0.077
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Multilayer0805 (2012 METRIC)Shielded100 uH20 %2 mA3.1 Ohms-- 55 C+ 125 C2512 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
NLCV32T-4R7M-EFD


RF Inductors - SMD 4.7uH 0.2ohms 620mA 3.2x2.5mm AEC-Q200
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TDK 1940
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AUD 0.1085
Multiples of: 5

Wirewound1210 (3225 METRIC)Unshielded4.7 uH20 %620 mA200 mOhms-- 40 C+ 105 C1546 MHzStandard3.2 mm2.5 mm2.4 mm-FerriteAEC - Q200NLCV25 - EFDReel , Cut Tape
BWCS00231715R68G00


RF Inductors - SMD 680nH RDC=2.20Ohms 190mA
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Pulse 1940
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AUD 0.101
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 2.35 mm x 1.73 mm x 1.52 mmUnshielded680 nH2 %190 mA2.2 Ohms190 mA- 40 C+ 125 C23188 MHzStandard2.35 mm1.73 mm1.52 mm Ceramic BWCSReel , Cut Tape
MLF2012E5R6JT000


RF Inductors - SMD 6 UH 5%
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TDK 1940
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AUD 0.1041
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Multilayer0805 (2012 METRIC)Shielded5.6 uH5 %15 mA600 mOhms-- 55 C+ 125 C5065 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
BWNC003729263R3K00


RF Inductors - SMD Chilisin RF inductor Wire Wound-High Current
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Pulse 1940
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AUD 0.1181
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                   BWNCReel , Cut Tape
LQW2UAS18NJ00L


RF Inductors - SMD
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Murata 1940
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AUD 0.1246
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Wirewound1008 (2520 METRIC)Unshielded18 nH5 %1 A110 mOhms-- 55 C+ 125 C502.5 GHzStandard2.62 mm2.45 mm1.83 mm-Air LQWReel , Cut Tape
MLF2012C180KTD25


RF Inductors - SMD 18uH 800mohms 5mA +/-10% Fer AEC-Q200
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TDK 1940
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AUD 0.1306
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Multilayer0805 (2012 METRIC)Shielded18 uH10 %5 mA800 mOhms-- 55 C+ 125 C3038 MHzStandard2 mm1.25 mm1.25 mm-FerriteAEC - Q200MLFReel , Cut Tape
AWCS00231715R22J00


RF Inductors - SMD Chilisin RF inductor Wire Wound-STD
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Pulse 1940
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AUD 0.1352
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 2.35 mm x 1.73 mm x 1.52 mmUnshielded220 nH5 %400 mA700 mOhms - 40 C+ 125 C50850 MHzStandard2.35 mm1.73 mm1.52 mm  AEC - Q200AWCSReel , Cut Tape
AWCS0023171515NJ00


RF Inductors - SMD Chilisin RF inductor Wire Wound-STD
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Pulse 1940
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AUD 0.1352
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 2.35 mm x 1.73 mm x 1.52 mmUnshielded15 nH5 %600 mA170 mOhms - 40 C+ 125 C503.4 GHzStandard2.35 mm1.73 mm1.52 mm  AEC - Q200AWCSReel , Cut Tape
NLV25T-180J-EF


RF Inductors - SMD 18uH 4.8ohms 130mA Wound Ferrite
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TDK 1940
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AUD 0.143
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Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded18 uH5 %130 mA4.8 Ohms-- 40 C+ 105 C2524 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
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