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
  
                         
LQP03TQ5N6J02D


RF Inductors - SMD PLEASE SEE MURATA'S SUGGESTED ALTERNATE LQP03HQ5N6J02D
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Murata 14501
Ships to you
between Thu. 16 Jul to Wed. 22 Jul Calender.png

AUD 0.0269
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Thin Film0201 (0603 METRIC)Unshielded5.6 nH5 %350 mA390 mOhms-- 55 C+ 125 C176 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
CIH10T47NJNC


Samsung CIH,High Frequency,0603,47nH,- ,7 paper,-5~5%
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Samsung 0
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AUD 0.0207
Multiples of: 4000

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BSCH0006030318NJ00


RF Inductors - SMD 0603 18nH
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Pulse 0
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AUD 0.0208
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 0.6 mm x 0.3 mm x 0.3 mmShielded18 nH5 % 810 mOhms170 mA- 55 C+ 125 C42.1 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic BSCHReel , Cut Tape
ATFC-0402-0N2-BT


RF Inductors - SMD
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ABRACON 0
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AUD 0.021
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Thin Film Chip Inductor0402 (1005 METRIC)Unshielded200 pH0.1 nH800 mA100 mOhms - 45 C+ 85 C1314 GHzStandard1 mm0.5 mm0.32 mm Ceramic ATFC - 0402Reel , Cut Tape
CIH10T39NJNC


Samsung CIH,High Frequency,0603,39nH,- ,7 paper,-5~5%
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Samsung 0
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AUD 0.0214
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LQP03HQ3N8C02D


RF Inductors - SMD
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Murata 0
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AUD 0.0204
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Thin Film0201 (0603 METRIC)Unshielded3.8 nH0.2 nH500 mA170 mOhms-- 55 C+ 125 C207 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
LCCI0402J47NGTAR


RF Inductors - SMD 47nH Tol 5% 0402 200 mA DCR=1.1 Ohms
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Kyocera AVX 0
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AUD 0.0219
Multiples of: 10000

Multilayer0402 (1005 METRIC)Unshielded47 nH5 %200 mA1.1 Ohms-- 40 C+ 85 C81.1 GHzStandard1 mm0.5 mm0.5 mm-  LCCIReel , Cut Tape
CW105550A-4N7J


RF Inductors - SMD 4.7nH 5 0.64A AEC-Q200
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Bourns 0
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AUD 0.0219
Multiples of: 1

Wirewound Unshielded4.7 nH5 %640 mA130 mOhms-- 40 C+ 125 C154.775 GHzStandard1 mm0.55 mm0.5 mm-CeramicAEC - Q200CW105550AReel
AIMC-0402-47NJ-T


RF Inductors - SMD FIXED IND 47NH 200MA 1.5 OHM SMD
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ABRACON 0
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AUD 0.022
Multiples of: 10000

Multilayer Ceramic Chip Inductor0402 (1005 METRIC)Shielded47 nH5 %200 mA1.5 Ohms - 55 C+ 125 C91 GHzStandard1 mm0.5 mm0.5 mm Ceramic AIMC - 0402Reel , Cut Tape
AISC-1008-R010J-T


RF Inductors - SMD FIXED IND 10NH 1A 80 MOHM SMD
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AUD 0.0355
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Wirewound1008 (2520 METRIC)Unshielded10 nH5 %1 A80 mOhms - 40 C+ 125 C504.1 GHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
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