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
  
                         
PE-0402CL1N2STT


RF Inductors - SMD 0402 1.2nH 400mA DCR=100mOhms RF
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Pulse 14140
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AUD 0.0264
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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
LQP02TQ0N9B02D


RF Inductors - SMD
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Murata 14132
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AUD 0.0841
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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
LQP03HQ0N9W02D


RF Inductors - SMD .9 NH
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Murata 14116
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AUD 0.1369
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Thin Film0201 (0603 METRIC)Unshielded900 pH0.05 nH1.1 A40 mOhms - 55 C+ 125 C2018 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
LQP02HQ0N7B02E


RF Inductors - SMD
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Murata 14113
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AUD 0.0891
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Thin Film01005 (0402 METRIC)Unshielded700 pH0.1 nH900 mA50 mOhms-- 55 C+ 125 C1415.5 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , Cut Tape
CWF1610-2R2K


RF Inductors - SMD Ind,1.6x1x1mm,2.2uH+/-10%,0.58A,non-shd
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Bourns 14107
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AUD 0.1353
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Wirewound0603 (1610 METRIC)Semi - Shielded2.2 uH10 %580 mA -- 40 C+ 125 C--Standard1.6 mm1 mm1 mm-Ferrite CWF1610Reel , Cut Tape
MLG0603P2N7CTD25


RF Inductors - SMD IND 0201 2.7nH Hi-Q AEC Q200 RF IND
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TDK 14098
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AUD 0.0396
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Multilayer0201 (0603 METRIC)Unshielded2.7 nH0.2 nH500 mA200 mOhms-- 55 C+ 125 C1410 GHzStandard0.6 mm0.3 mm0.3 mm-CeramicAEC - Q200MLG - PReel , Cut Tape
AIMC-Q0201HQ-2N7C-T


RF Inductors - SMD IND 2.7nH 0.5A 200m?
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Abracon 13923
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AUD 0.0534
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Multilayer Ceramic Chip Inductor0201 (0603 METRIC)Shielded2.7 nH0.2 nH500 mA200 mOhms - 55 C+ 125 C1410 GHzStandard0.6 mm0.3 mm0.3 mm Ceramic AIMC - Q0201HQReel , Cut Tape
MLG1005S1N1BTD25


RF Inductors - SMD IND 0402 1.1nH StdQ AEC Q200 RF IND
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TDK 13876
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AUD 0.0781
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Multilayer0402 (1005 METRIC)Unshielded1.1 nH0.1 nH1 A100 mOhms-- 55 C+ 125 C719.3 GHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
LQP03TN22NHZ2D


RF Inductors - SMD
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Murata 13851
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AUD 0.0319
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Thin Film0201 (0603 METRIC)Unshielded22 nH3 %150 mA1.9 Ohms-- 55 C+ 125 C122.2 GHzStandard0.6 mm0.3 mm0.3 mm-FerriteAEC - Q200LQPReel , Cut Tape
MHQ0603P3N5BTD25


RF Inductors - SMD 0201 3.5nH Tol 0.1nH AEC-Q200
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TDK 13806
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AUD 0.0742
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Multilayer0201 (0603 METRIC)Unshielded3.5 nH0.1 nH500 mA250 mOhms-- 55 C+ 125 C169.5 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
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