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
  
                         
LQP02TQ2N8B02D


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 19400
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AUD 0.0996
Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded2.8 nH0.1 nH360 mA450 mOhms-- 55 C+ 125 C1010 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
LQW18AS5N6G0ZD


RF Inductors - SMD 5.6 NH 2%
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Murata 19400
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AUD 0.1044
Multiples of: 4000

Wirewound0603 (1608 METRIC)Unshielded5.6 nH2 %700 mA75 mOhms-- 40 C+ 125 C264.76 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQW15AN1N3C8ZD


RF Inductors - SMD 1.3 NH
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Murata 19400
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AUD 0.12
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Wirewound0402 (1005 METRIC)Unshielded1.3 nH0.2 nH3.15 A12 mOhms-- 55 C+ 125 C2018 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQW15AN5N1B8ZD


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 19400
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AUD 0.13
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Wirewound0402 (1005 METRIC)Unshielded5.1 nH0.1 nH1.77 A40 mOhms-- 55 C+ 125 C358 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
LQG15WZ1N5B02D


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 19400
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AUD 0.1361
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded1.5 nH0.1 nH1 A40 mOhms-- 55 C+ 125 C2311 GHzStandard1 mm0.6 mm0.5 mm-Air LQGReel , Cut Tape
NLV32T-470J-EFD


RF Inductors - SMD 47uH 7.0ohms 60mA Wound Fer AEC-Q200
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TDK 19400
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AUD 0.1465
Multiples of: 2000

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded47 uH5 %60 mA7 Ohms-- 40 C+ 105 C3015 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
Hot MLF1005GR39JTD25


RF Inductors - SMD 0402 0.39uH 5% AEC-Q200
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TDK 19400
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AUD 0.1475
Multiples of: 1

Multilayer0402 (1005 METRIC)Shielded390 nH5 %50 mA410 mOhms-- 55 C+ 125 C30600 MHzStandard1 mm0.5 mm0.5 mm-FerriteAEC - Q200MLFReel , Cut Tape
IWC0603BR22R-3G


RF Inductors - SMD 0603 220nH 2% 200mA
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Laird Performance Materials 19400
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AUD 0.1532
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Wirewound1.8 mm x 1.12 mm x 1.02 mmUnshielded220 nH2 %200 mA2.02 Ohms-- 40 C+ 125 C25900 MHzStandard1.8 mm1.12 mm1.02 mm-Ceramic IWC0603Reel , Cut Tape
LQG15WH82NG02D


RF Inductors - SMD Fixed IND 82nH 160mA POWRTRN
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Murata 19400
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AUD 0.1614
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded82 nH2 %160 mA2.3 Ohms-- 55 C+ 125 C22900 MHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , 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 19400
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AUD 0.1667
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
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