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
  
                         
B82496C3829J


RF Inductors - SMD 8.2nH 650mA 5% 1.6x0.8mm SMD
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TDK 14153
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AUD 0.2204
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Wirewound0603 (1608 METRIC)Unshielded8.2 nH5 %650 mA180 mOhms-- 55 C+ 150 C146 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200SIMID - CReel , Cut Tape
LQP03TQ1N5W02D


RF Inductors - SMD 1.5nH 650mA 0201 (0603 metric) SUGGESTED ALT LQP03HQ1N5W02D
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Murata 14152
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AUD 0.0316
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded1.5 nH0.05 nH650 mA100 mOhms-- 55 C+ 125 C1715 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP02TQ8N2H02D


RF Inductors - SMD
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Murata 14132
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AUD 0.0057
Multiples of: 10

Thin Film01005 (0402 METRIC)Unshielded8.2 nH3 %190 mA1.6 Ohms-- 55 C+ 125 C106.6 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
CWF1610-6R8K


RF Inductors - SMD Ind,1.6x1x1mm,6.8uH+/-10%,0.34A,non-shd
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Bourns 14111
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AUD 0.0891
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Wirewound0603 (1610 METRIC)Semi - Shielded6.8 uH10 %340 mA -- 40 C+ 125 C--Standard1.6 mm1 mm1 mm-Ferrite CWF1610Reel , Cut Tape
LQW15AN3N9B8ZD


RF Inductors - SMD
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Murata 14105
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AUD 0.1265
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded3.9 nH0.1 nH1.95 A30 mOhms-- 55 C+ 125 C3510 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
MHQ0603P1N0CT000


RF Inductors - SMD IND 0201 1.0nH S-HQ SMD RF IND
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TDK 14091
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AUD 0.0378
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded1 nH0.2 nH1 A70 mOhms-- 55 C+ 125 C-19.3 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
LQP02HQ47NH02E


RF Inductors - SMD
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Murata 14082
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AUD 0.109
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Thin Film01005 (0402 METRIC)Unshielded47 nH3 %100 mA4 Ohms-- 55 C+ 125 C82.1 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP02HQ36NH02E


RF Inductors - SMD
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Murata 14077
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AUD 0.109
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Thin Film01005 (0402 METRIC)Unshielded36 nH3 %110 mA3.6 Ohms-- 55 C+ 125 C92.4 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , Cut Tape
MLG0603P62NHT000


RF Inductors - SMD IND 0201 62nH Hi-Q SMD RF IND
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TDK 14074
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AUD 0.0208
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded62 nH3 %100 mA3.5 Ohms-- 55 C+ 125 C101.6 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
LQP03TN4N1B02D


RF Inductors - SMD 4.1 NH +/-0.1NH
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Murata 14065
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AUD 0.0088
Multiples of: 50

Thin Film0201 (0603 METRIC)Unshielded4.1 nH0.1 nH350 mA400 mOhms - 55 C+ 125 C145.3 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
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