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
  
                         
LQW18AN27NG10D


RF Inductors - SMD 27 NH 2%
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Murata 14752
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AUD 0.099
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded27 nH2 %590 mA116 mOhms-- 55 C+ 125 C422.8 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
MLF1005GR68KT000


RF Inductors - SMD 1mm x 0.5mm x 0.5mm, -55 to +125 degC, 45mA, 0.68?H, 550mohm
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TDK 14752
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AUD 0.1225
Multiples of: 1

Multilayer0402 (1005 METRIC)Shielded680 nH10 %45 mA550 mOhms-- 55 C+ 125 C30360 MHzStandard1 mm0.5 mm0.5 mm-Ferrite MLFReel , Cut Tape
LQW15AW56NJ80D


RF Inductors - SMD Fixed IND 56nH 480mA NONAUTO
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Murata 14749
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AUD 0.163
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded56 nH5 %480 mA520 mOhms-- 55 C+ 125 C332.1 GHzStandard1.02 mm0.61 mm0.61 mm-  LQWReel , Cut Tape
LQP02TN3N9B02D


RF Inductors - SMD
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Murata 14744
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AUD 0.0116
Multiples of: 50

Thin Film01005 (0402 METRIC)Unshielded3.9 nH0.1 nH180 mA1.3 Ohms - 55 C+ 125 C87.5 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
LQW15AN2N9B00D


RF Inductors - SMD 2.9 NH +-.1NH
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Murata 14744
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AUD 0.0306
Multiples of: 20

Wirewound0402 (1005 METRIC)Unshielded2.9 nH0.1 nH750 mA70 mOhms-- 55 C+ 125 C2015 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQP02HQ16NH02E


RF Inductors - SMD
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Murata 14705
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AUD 0.1192
Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded16 nH3 %170 mA1.53 Ohms-- 55 C+ 125 C144 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP03HQ4N5H02D


RF Inductors - SMD Fixed IND 4.5nH 400mA NONAUTO
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Murata 14690
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AUD 0.0836
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded4.5 nH3 %400 mA250 mOhms-- 55 C+ 125 C207 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
LQP02TQ0N9B02D


RF Inductors - SMD
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Murata 14685
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AUD 0.0874
Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded900 pH0.1 nH580 mA150 mOhms-- 55 C+ 125 C1016.6 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
PE-0402CL1N2STT


RF Inductors - SMD 0402 1.2nH 400mA DCR=100mOhms RF
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Pulse 14674
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AUD 0.0293
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded1.2 nH0.3 nH400 mA100 mOhms-- 55 C+ 125 C810 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
LQG15WH68NG02D


RF Inductors - SMD Fixed IND 68nH 160mA POWRTRN
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Murata 14652
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AUD 0.1449
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded68 nH2 %160 mA2 Ohms-- 55 C+ 125 C221.1 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
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