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
  
                         
MHQ0402PSA2N0CT000


RF Inductors - SMD 01005, 2.0nH +-0.2nH S-HQ SMD RF IND
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TDK 19293
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AUD 0.0525
Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded2 nH0.2 nH400 mA400 mOhms-- 55 C+ 125 C1012.76 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
MHQ0402PSA1N2CT000


RF Inductors - SMD 01005, 1.2nH +-0.2nH S-HQ SMD RF IND
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TDK 19293
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AUD 0.0525
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Multilayer01005 (0402 METRIC)Unshielded1.2 nH0.2 nH500 mA200 mOhms-- 55 C+ 125 C1016.72 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
MHQ0402PSA1N9CT000


RF Inductors - SMD 01005, 1.9nH +-0.2nH S-HQ SMD RF IND
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TDK 19283
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AUD 0.0525
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Multilayer01005 (0402 METRIC)Unshielded1.9 nH0.2 nH400 mA400 mOhms-- 55 C+ 125 C1012.69 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQW15AN2N5B8ZD


RF Inductors - SMD
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Murata 19283
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AUD 0.1306
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Wirewound0402 (1005 METRIC)Unshielded2.5 nH0.1 nH2.1 A30 mOhms-- 55 C+ 125 C3015.5 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
PE-0402CL820JTT


RF Inductors - SMD 0402 82nH 150mA DCR=2400mOhms RF
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Pulse 19279
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AUD 0.0293
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded82 nH5 %150 mA2.4 Ohms-- 55 C+ 125 C8750 MHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
LQP02TN4N1B02D


RF Inductors - SMD
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Murata 19273
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AUD 0.0446
Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded4.1 nH0.1 nH180 mA1.3 Ohms - 55 C+ 125 C87.5 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
MLG0402P0N3CT000


RF Inductors - SMD IND 01005 0.3nH Hi-Q SMD RF IND
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TDK 19254
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AUD 0.0252
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Multilayer01005 (0402 METRIC)Shielded300 pH0.2 nH350 mA100 mOhms-- 55 C+ 125 C-20 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MLG - PReel , Cut Tape
MCLA1005V2-200-R


RF Inductors - SMD 20 NH 5% AEC-Q200
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Eaton 19253
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AUD 0.033
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded20 nH0.3 nH300 mA600 mOhms-- 40 C+ 125 C82 GHzStandard1 mm0.5 mm0.5 mm- AEC - Q200MCLAReel , Cut Tape
MHQ0402PSA2N9BT000


RF Inductors - SMD 01005, 2.9nH +-0.1nH S-HQ SMD RF IND
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TDK 19249
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AUD 0.033
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Multilayer01005 (0402 METRIC)Unshielded2.9 nH0.1 nH250 mA600 mOhms-- 55 C+ 125 C1010.49 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQW15AN3N5B8ZD


RF Inductors - SMD 3.5 NH +-0.1 NH
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Murata 19223
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AUD 0.1155
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded3.5 nH0.1 nH1.95 A30 mOhms-- 55 C+ 125 C3010 GHzStandard1 mm0.6 mm0.5 mm- AEC - Q200LQWReel , Cut Tape
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