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
  
                         
LQP02TN2N0B02D


RF Inductors - SMD
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Murata 19176
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AUD 0.0495
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Thin Film01005 (0402 METRIC)Unshielded2 nH0.1 nH200 mA750 mOhms - 55 C+ 125 C89 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
MHQ0402PSA5N6JT000


RF Inductors - SMD 01005, 5.6nH +-5% S-HQ SMD RF IND
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TDK 19172
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AUD 0.0525
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Multilayer01005 (0402 METRIC)Unshielded5.6 nH5 %200 mA800 mOhms-- 55 C+ 125 C107.49 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQP02TQ9N1J02D


RF Inductors - SMD
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Murata 19167
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AUD 0.0625
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Thin Film01005 (0402 METRIC)Unshielded9.1 nH5 %170 mA1.7 Ohms-- 55 C+ 125 C105.9 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
LCCI0603JR10GTAR


RF Inductors - SMD 100nH Tol 5% 0603 30 0mA DCR=1 Ohms
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Kyocera AVX 19165
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AUD 0.0582
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Multilayer0603 (1608 METRIC)Unshielded100 nH5 %300 mA1 Ohms-- 40 C+ 85 C12600 MHzStandard1.6 mm0.8 mm0.8 mm-  LCCIReel , Cut Tape
LQW18AS4N7J00D


RF Inductors - SMD
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Murata 19155
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AUD 0.0868
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Wirewound0603 (1608 METRIC)Unshielded4.7 nH5 %700 mA116 mOhms-- 40 C+ 125 C205.8 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
IWC0402B39NR-3G


RF Inductors - SMD 0402 39nH 2% 200mA
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Laird Performance Materials 19141
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AUD 0.1659
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Wirewound1.19 mm x 0.66 mm x 0.7 mmUnshielded39 nH2 %200 mA550 mOhms-- 40 C+ 125 C252.1 GHzStandard1.19 mm0.7 mm0.66 mm-Ceramic IWC0402Reel , Cut Tape
MHQ0402PSA1N6CT000


RF Inductors - SMD 01005, 1.6nH +-0.2nH S-HQ SMD RF IND
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TDK 19132
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AUD 0.0525
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Multilayer01005 (0402 METRIC)Unshielded1.6 nH0.2 nH400 mA300 mOhms-- 55 C+ 125 C1015.27 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
MHQ1005P9N1JT000


RF Inductors - SMD IND 0402 9.1nH S-HQ SMD RF IND
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TDK 19128
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AUD 0.0891
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Multilayer0402 (1005 METRIC)Unshielded9.1 nH5 %550 mA170 mOhms-- 55 C+ 125 C234.5 GHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
BSCH001005054N3SCS


RF Inductors - SMD 4.3nH RDC=0.18Ohms 400mA
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Pulse 19109
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AUD 0.0152
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 1 mm x 0.5 mm x 0.5 mmShielded4.3 nH0.3 nH 180 mOhms400 mA- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm Ceramic BSCHReel , Cut Tape
Hot LQG15HS39NJ02D


RF Inductors - SMD 39 NH 5%
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Murata 17169
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AUD 0.0081
Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded39 nH5 %300 mA650 mOhms - 55 C+ 125 C81.2 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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