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
  
                         
LQG15HN8N2H02D


RF Inductors - SMD 8.2NH 500MA
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Murata 51398
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AUD 0.033
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded8.2 nH3 %500 mA250 mOhms-- 55 C+ 125 C83.6 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
CIGT201208EH1R0MNE


RF Inductors - SMD CIGT,Thin Film,0805,1.0uH,0.8?,7 embossed,-20 20%
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Samsung 49939
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AUD 0.1386
Multiples of: 1

Thin Film Unshielded1 uH20 %3.1 A55 mOhms3.5 A- 40 C+ 125 C--Standard2 mm1.25 mm0.8 mm-  CIGTReel , Cut Tape
LQP03HQ4N3H02D


RF Inductors - SMD 4.3 NH 3%
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Murata 49295
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AUD 0.0332
Multiples of: 20

Thin Film0201 (0603 METRIC)Unshielded4.3 nH3 %500 mA170 mOhms-- 55 C+ 125 C207 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
LQW15AN3N3G8ZD


RF Inductors - SMD 3.3 NH 2%
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Murata 48500
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AUD 0.1206
Multiples of: 10000

Wirewound0402 (1005 METRIC)Unshielded3.3 nH2 %2 A30 mOhms-- 55 C+ 125 C3014 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQG15HZ10NH02D


RF Inductors - SMD 10 NH 3%
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Murata 48034
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AUD 0.0485
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded10 nH3 %500 mA260 mOhms-- 55 C+ 125 C83.4 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQW15AN8N6G8ZD


RF Inductors - SMD
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Murata 47950
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AUD 0.1188
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded8.6 nH2 %1.42 A70 mOhms-- 55 C+ 125 C6.56.5 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQW15AN18NH00D


RF Inductors - SMD 18 NH 3%
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Murata 47933
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AUD 0.0742
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded18 nH3 %370 mA270 mOhms-- 55 C+ 125 C254.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQP03TG0N6B02D


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 47891
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AUD 0.0148
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded600 pH0.1 nH850 mA80 mOhms - 55 C+ 125 C1118 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP03TN6N8H02D


RF Inductors - SMD 6.8 NH 3%
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Murata 46220
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AUD 0.0192
Multiples of: 50

Thin Film0201 (0603 METRIC)Unshielded6.8 nH3 %300 mA600 mOhms-- 55 C+ 125 C143.9 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP03TG0N5B02D


RF Inductors - SMD .5 NH +-.1NH
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Murata 38098
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AUD 0.0148
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded500 pH0.1 nH850 mA80 mOhms - 55 C+ 125 C2018 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
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