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
  
                         
Hot LQP03TN2N2B02D


RF Inductors - SMD 2.2 NH
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Murata 263161
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AUD 0.013
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded2.2 nH0.1 nH600 mA150 mOhms - 55 C+ 125 C1411 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
AISC-0402-12NG-T


RF Inductors - SMD 12 NH 2%
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Abracon 135800
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AUD 0.1785
Multiples of: 10000

Ceramic Wirewound RF Inductor0402 (1005 METRIC)Unshielded12 nH2 %640 mA120 mOhms   263.6 GHzStandard1.1 mm0.6 mm0.66 mm Ceramic AISC - 0402Reel , Cut Tape
BSCH0010050510NJCS


RF Inductors - SMD 1005 10nH
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Pulse 134351
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AUD 0.0198
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 1 mm x 0.5 mm x 0.5 mmShielded10 nH5 % 260 mOhms300 mA- 55 C+ 125 C83.9 GHzStandard1 mm0.5 mm0.5 mm-Ceramic BSCHReel , Cut Tape
LQW15AN2N6G8ZD


RF Inductors - SMD
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 126950
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AUD 0.1323
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Wirewound0402 (1005 METRIC)Unshielded2.6 nH2 %1.95 A35 mOhms-- 55 C+ 125 C3014.5 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
NLCV32T-2R2M-EFR


RF Inductors - SMD 2.2uH 138mohms 1.2A 125C Wound Ferrite
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TDK 125990
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AUD 0.1254
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded2.2 uH20 %770 mA130 mOhms-- 40 C+ 105 C1068 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFRReel , Cut Tape
BSCH000603038N2J00


RF Inductors - SMD 0603 8.2nH
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Pulse 123990
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AUD 0.0173
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 0.6 mm x 0.3 mm x 0.3 mmShielded8.2 nH5 % 450 mOhms230 mA- 55 C+ 125 C43.4 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic BSCHReel , Cut Tape
CIGT201208EHR47MNE


RF Inductors - SMD CIGT,Thin Film,0805,0.47uH,0.8?,7 embossed,-20 20%
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SAMSUNG 119964
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AUD 0.132
Multiples of: 1

Thin Film Unshielded470 nH20 %4.1 A35 mOhms4.3 A- 40 C+ 125 C--Standard2 mm1.25 mm0.8 mm-  CIGTReel , Cut Tape
LQG15HS33NJ02D


RF Inductors - SMD 33 NH 5%
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Murata 108064
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AUD 0.0264
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded33 nH5 %350 mA580 mOhms-- 55 C+ 125 C81.6 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQG15HS4N7B02D


RF Inductors - SMD 4.7 NH +/-0.1NH
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Murata 107789
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AUD 0.0413
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Multilayer0402 (1005 METRIC)Unshielded4.7 nH0.1 nH700 mA160 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQG15HS4N7S02D


RF Inductors - SMD 4.7 NH 3%
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Murata 99157
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AUD 0.0264
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded4.7 nH0.3 nH700 mA160 mOhms - 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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