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
  
                         
LQG15WH2N7C02D


RF Inductors - SMD
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Murata 19711
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AUD 0.0848
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded2.7 nH0.2 nH900 mA70 mOhms-- 55 C+ 125 C236.5 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
MLG0603P15NHT000


RF Inductors - SMD IND 0201 15nH Hi-Q SMD RF IND
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TDK 19691
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AUD 0.0046
Multiples of: 100

Multilayer0201 (0603 METRIC)Unshielded15 nH3 %250 mA1.2 Ohms-- 55 C+ 125 C143.7 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
MLF1608DR15KTA00


RF Inductors - SMD 1.6mm x 0.8mm x 0.8mm, -55 to +125 degC, 200mA, 0.15?H, 450mohm
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TDK 19604
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AUD 0.0792
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Multilayer0603 (1608 METRIC)Shielded150 nH10 %200 mA450 mOhms-- 55 C+ 125 C15500 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
BSCQ000603032N7B00


RF Inductors - SMD 2.7nH RDC=0.32Ohms 400mA
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Pulse 19585
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AUD 0.0173
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 0.6 mm x 0.3 mm x 0.3 mmShielded2.7 nH0.1 nH400 mA320 mOhms400 mA- 55 C+ 125 C1410 GHzStandard0.6 mm0.3 mm0.3 mm Ceramic BSCQReel , Cut Tape
MLG0603P7N5HT000


RF Inductors - SMD IND 0201 7.5nH Hi-Q SMD RF IND
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TDK 19571
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AUD 0.0231
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded7.5 nH3 %300 mA800 mOhms-- 55 C+ 125 C145.4 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
LQP03HQ68NH02D


RF Inductors - SMD
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Murata 19510
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AUD 0.1089
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded68 nH3 %100 mA5 Ohms-- 55 C+ 125 C121.1 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
AC4842R-27NK


RF Inductors - SMD AC,4.83x3.81x4.2mm,27nH+/-10%,3.5A,SMD
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Bourns 19497
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AUD 0.1854
Multiples of: 1

Air Coil Inductor2015 (4838 METRIC) 27 nH10 %3.5 A4 mOhms - 25 C+ 125 C1002.7 GHzStandard4.83 mm3.81 mm4.2 mm   AC4842RReel , Cut Tape
LQW15AN56NG00D


RF Inductors - SMD 56 NH 2%
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Murata 19400
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AUD 0.0789
Multiples of: 10000

Wirewound0402 (1005 METRIC)Unshielded56 nH2 %200 mA1.17 Ohms-- 55 C+ 125 C252.8 GHzStandard1 mm0.5 mm0.5 mm-  LQWReel , Cut Tape
LQG15HS39NH02D


RF Inductors - SMD
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Murata 19268
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AUD 0.033
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Multilayer0402 (1005 METRIC)Unshielded39 nH3 %300 mA650 mOhms-- 55 C+ 125 C81.2 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
PE-0603CLH2R2STS


RF Inductors - SMD 0603 2.2uH 750mA DCR=312mOhms RF
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Pulse 0
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AUD 0.127
Multiples of: 1

Multilayer0603 (1608 METRIC)Shielded2.2 uH-750 mA312 mOhms400 mA- 40 C+ 85 C-95 MHzStandard1.6 mm0.8 mm0.8 mm-Ceramic PE - 0603CLHReel , Cut Tape
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