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
  
                         
LQW03AW10NJ00D


RF Inductors - SMD
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Murata 8975
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AUD 0.5137
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Wirewound0201 (0603 METRIC)Unshielded10 nH5 %250 mA460 mOhms-- 55 C+ 125 C377.2 GHzStandard0.53 mm0.4 mm0.4 mm-  LQWReel , Cut Tape
MLG1005SR22JT000


RF Inductors - SMD IND 0402 220nH StdQ SMD RF IND
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TDK 8972
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AUD 0.007
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Multilayer0402 (1005 METRIC)Unshielded220 nH5 %100 mA4.2 Ohms-- 55 C+ 125 C8500 MHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , Cut Tape
CIGT201608EHR47MNE


RF Inductors - SMD CIGT,Thin Film,0806,0.47uH,0.8?,7 embossed,-20 20%
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SAMSUNG 8972
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AUD 0.139
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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
MLG1005SR12JTD25


RF Inductors - SMD IND 0402 120nH StdQ AEC Q200 RF IND
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TDK 8969
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AUD 0.0852
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Multilayer0402 (1005 METRIC)Unshielded120 nH5 %150 mA2.2 Ohms-- 55 C+ 125 C8800 MHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
LQG15WH20NJ02D


RF Inductors - SMD Fixed IND 20nH 260mA POWRTRN
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Murata 8964
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AUD 0.065
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Multilayer0402 (1005 METRIC)Unshielded20 nH5 %260 mA1.1 Ohms-- 55 C+ 125 C202.1 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQW15CAR56J00D


RF Inductors - SMD
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Murata 8963
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AUD 0.3209
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Wirewound0402 (1005 METRIC)Unshielded560 nH5 %270 mA1 Ohms-- 40 C+ 125 C-900 MHzStandard1 mm0.5 mm0.5 mm-  LQWReel , Cut Tape
B82422T1473K


RF Inductors - SMD 47uH 60mA 10% 3.2x2.5mm SMD
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TDK 8962
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AUD 0.2875
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Wirewound1210 (3225 METRIC)Unshielded47 uH10 %60 mA7 Ohms-- 55 C+ 125 C2715 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422TReel , Cut Tape
LQG15HH7N5G02D


RF Inductors - SMD
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Murata 8951
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AUD 0.12
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Multilayer Unshielded7.5 nH2 %550 mA240 mOhms - 55 C+ 125 C84.2 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQG15HZ18NG02D


RF Inductors - SMD
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Murata 8948
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AUD 0.103
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Multilayer0402 (1005 METRIC)Unshielded18 nH2 %400 mA360 mOhms-- 55 C+ 125 C82.2 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQW03AW8N7J00D


RF Inductors - SMD
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Murata 8941
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AUD 0.4866
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Wirewound0201 (0603 METRIC)Unshielded8.7 nH5 %290 mA220 mOhms-- 55 C+ 125 C467.5 GHzStandard0.53 mm0.4 mm0.4 mm-  LQWReel , Cut Tape
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