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
  
                         
AIML-1206-100K-T


RF Inductors - SMD 10 UH +/-10%
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ABRACON 29107
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AUD 0.1627
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Multilayer Ferrite Chip Inductor1206 (3216 METRIC)Shielded10 uH10 %25 mA800 mOhms - 55 C+ 125 C5528 MHzStandard3.2 mm1.6 mm1.1 mm Ferrite AIML - 1206Reel , Cut Tape
LQP02HQ3N0B02E


RF Inductors - SMD
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Murata 18871
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AUD 0.1
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Thin Film01005 (0402 METRIC)Unshielded3 nH0.1 nH450 mA200 mOhms - 55 C+ 125 C148.5 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQG15WH68NJ02D


RF Inductors - SMD Fixed IND 68nH 160mA POWRTRN
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Murata 18868
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AUD 0.0807
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Multilayer0402 (1005 METRIC)Unshielded68 nH5 %160 mA2 Ohms-- 55 C+ 125 C221.1 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
MCLA1005V2-3R0-R


RF Inductors - SMD MCLA Auto Chip IND 1005 3.0nH 2 Pads
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Eaton 18861
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AUD 0.0385
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Multilayer0402 (1005 METRIC)Unshielded3 nH5 %300 mA200 mOhms-- 40 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm- AEC - Q200MCLAReel , Cut Tape
AIMC-Q0402-4N7B-T


RF Inductors - SMD IND 4.7nH 0.7A 20m?
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Abracon 18860
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AUD 0.0541
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Multilayer Ceramic Chip Inductor0402 (1005 METRIC)Shielded4.7 nH0.1 nH700 mA200 mOhms - 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm Ceramic AIMC - Q0402Reel , Cut Tape
PE-0402CL101JTT


RF Inductors - SMD 0402 100nH 150mA DCR=26000mOhms RF
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Pulse 18851
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AUD 0.0315
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Multilayer0402 (1005 METRIC)Unshielded100 nH5 %150 mA2.6 Ohms-- 55 C+ 125 C8700 MHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
MHQ0402PSA4N0CT000


RF Inductors - SMD 01005, 4.0nH +-0.2nH S-HQ SMD RF IND
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TDK 18847
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AUD 0.0525
Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded4 nH0.2 nH200 mA800 mOhms-- 55 C+ 125 C108.8 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
MHQ0402PSA1N7BT000


RF Inductors - SMD 01005, 1.7nH +-0.1nH S-HQ SMD RF IND
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TDK 18841
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AUD 0.009
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Multilayer01005 (0402 METRIC)Unshielded1.7 nH0.1 nH400 mA400 mOhms-- 55 C+ 125 C1014.22 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LCCI0402S5N6GTAR


RF Inductors - SMD 5.6nH Tol 0.3nH 0402 600mA DCR=0.23 Ohms
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Kyocera AVX 18837
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AUD 0.0126
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Multilayer0402 (1005 METRIC)Unshielded5.6 nH0.3 nH600 mA250 mOhms-- 40 C+ 85 C84.5 GHzStandard1 mm0.5 mm0.5 mm-Ceramic LCCIReel , Cut Tape
MHQ0402PSA1N5ST000


RF Inductors - SMD 01005, 1.5nH +-0.3nH S-HQ SMD RF IND
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TDK 18833
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AUD 0.026
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Multilayer01005 (0402 METRIC)Unshielded1.5 nH0.3 nH400 mA200 mOhms-- 55 C+ 125 C1014.74 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
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