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
  
                         
LQP02TN2N1B02D


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 15583
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AUD 0.0485
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Thin Film01005 (0402 METRIC)Unshielded2.1 nH0.1 nH200 mA750 mOhms - 55 C+ 125 C89 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
LQP03TG2N5B02D


RF Inductors - SMD
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Murata 15557
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AUD 0.0165
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Thin Film0201 (0603 METRIC)Unshielded2.5 nH0.1 nH450 mA250 mOhms - 55 C+ 125 C1311 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQW15AN11NH00D


RF Inductors - SMD
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Murata 15533
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AUD 0.0785
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Wirewound0402 (1005 METRIC)Unshielded11 nH3 %500 mA140 mOhms-- 55 C+ 125 C305.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
AIMC-0603-3N3S-T


RF Inductors - SMD FIXED IND 3.3NH 500MA 120 MOHM
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ABRACON 15520
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AUD 0.041
Multiples of: 4000

Multilayer Ceramic Chip Inductor0603 (1608 METRIC)Shielded3.3 nH0.3 nH500 mA150 mOhms - 55 C+ 125 C136 GHzStandard1.6 mm0.8 mm0.8 mm Ceramic AIMC - 0603Reel , Cut Tape
MLF2012A1R8KTD25


RF Inductors - SMD 1.8uH 450mohms 80mA +/-10% Fer AEC-Q200
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TDK 15520
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AUD 0.1014
Multiples of: 4000

Multilayer0805 (2012 METRIC)Shielded1.8 uH10 %80 mA450 mOhms-- 55 C+ 125 C45130 MHzStandard2 mm1.25 mm0.85 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQW2BAS22NJ00L


RF Inductors - SMD 22 NH 5%
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Murata 15520
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AUD 0.1247
Multiples of: 2000

Wirewound0805 (2015 METRIC)Unshielded22 nH5 %500 mA220 mOhms-- 55 C+ 125 C552.6 GHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
NLFV32T-220K-EF


RF Inductors - SMD 3.2mm x 2.5mm x 2.2mm, -40 to +105 degC, 120mA, 22?H, 480mohm
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TDK 15520
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AUD 0.1408
Multiples of: 2000

Wirewound1210 (3225 METRIC)Shielded22 uH10 %120 mA400 mOhms-- 40 C+ 105 C--Standard3.2 mm2.5 mm2.2 mm-Ferrite NLFV32 - EFReel , Cut Tape
ILSB0805ER2R2K


RF Inductors - SMD 2.2uH 10%
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Vishay 15512
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AUD 0.104
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Established Reliability0805 (2012 METRIC)Shielded2.2 uH10 %30 mA650 mOhms-- 55 C+ 125 C4558 MHzStandard2 mm1.25 mm0.9 mm-  ILSB - 0805Reel , Cut Tape
LQW18ANR47G00D


RF Inductors - SMD .47 UH 2%
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Murata 15238
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AUD 0.0595
Multiples of: 10

Wirewound0603 (1608 METRIC)Unshielded470 nH2 %75 mA7 Ohms-- 55 C+ 125 C30700 MHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQW15AN3N3B80D


RF Inductors - SMD 3.3 NH +-.1NH
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Murata 14889
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AUD 0.0737
Multiples of: 10

Wirewound0402 (1005 METRIC)Unshielded3.3 nH0.1 nH2 A30 mOhms-- 55 C+ 125 C3014 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
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