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
  
                         
LQW03AW3N9C00D


RF Inductors - SMD
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Murata 13911
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AUD 0.4917
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Wirewound0201 (0603 METRIC)Unshielded3.9 nH0.2 nH650 mA70 mOhms-- 55 C+ 125 C4811 GHzStandard0.53 mm0.4 mm0.4 mm-  LQWReel , Cut Tape
LQP03TQ1N9B02D


RF Inductors - SMD 1.9nH 650mA 0201 (0603 metric) SUGGESTED ALT LQP03HQ1N9B02D
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Murata 13900
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AUD 0.0336
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Thin Film0201 (0603 METRIC)Unshielded1.9 nH0.1 nH650 mA100 mOhms-- 55 C+ 125 C1712.5 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP02TN1N4B02D


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 13900
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AUD 0.0424
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Thin Film01005 (0402 METRIC)Unshielded1.4 nH0.1 nH220 mA600 mOhms - 55 C+ 125 C811.5 GHzStandard0.4 mm0.2 mm0.2 mm Ferrite LQPReel , Cut Tape
MLG1005S1N6ST000


RF Inductors - SMD IND 0402 1.6nH StdQ SMD RF IND
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TDK 13877
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AUD 0.0644
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Multilayer0402 (1005 METRIC)Unshielded1.6 nH0.3 nH1 A120 mOhms-- 55 C+ 125 C79.4 GHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , Cut Tape
MLG0603S2N0BT000


RF Inductors - SMD IND 0201 2.0nH StdQ SMD RF IND
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TDK 13873
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AUD 0.0485
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Multilayer0201 (0603 METRIC)Unshielded2 nH0.1 nH400 mA250 mOhms-- 55 C+ 125 C49.8 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLGReel , Cut Tape
PE-0402CL3N6STT


RF Inductors - SMD 0402 3.6nH 300mA DCR=200mOhms RF
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Pulse 13871
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AUD 0.0264
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Multilayer0402 (1005 METRIC)Unshielded3.6 nH0.3 nH300 mA200 mOhms-- 55 C+ 125 C84 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
LQP03HQ0N5C02D


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 13871
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AUD 0.0742
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Thin Film0201 (0603 METRIC)Unshielded500 pH0.2 nH1.1 A40 mOhms-- 55 C+ 125 C2020 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
L02012R2BHSTR


RF Inductors - SMD 2.2nH
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Kyocera AVX 13850
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AUD 0.462
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Thin Film0201 (0603 METRIC)Unshielded2.2 nH0.1 nH200 mA600 mOhms-- 55 C+ 125 C718 GHzStandard0.6 mm0.325 mm0.225 mm-  Accu - LReel , Cut Tape
LQW15AN20NJ8ZD


RF Inductors - SMD
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Murata 13841
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AUD 0.1212
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Wirewound0402 (1005 METRIC)Unshielded20 nH5 %800 mA186 mOhms-- 55 C+ 125 C304.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
CIGT252008LM2R2MNE


RF Inductors - SMD CIGT,Thin Film,1008,2.2uH,0.8?,7 embossed,-20 20%
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SAMSUNG 13765
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AUD 0.1147
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Thin Film Shielded2.2 uH20 %2 A97 mOhms1.9 A- 40 C+ 125 C--Standard2.5 mm2 mm0.8 mm-Metal Composite CIGTReel , Cut Tape
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