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
  
                         
MHQ0603P2N4CT000


RF Inductors - SMD IND 0201 2.4nH S-HQ SMD RF IND
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TDK 13628
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AUD 0.0667
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded2.4 nH0.2 nH700 mA150 mOhms-- 55 C+ 125 C1611.7 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
MLG0603S2N0ST000


RF Inductors - SMD IND 0201 2.0nH StdQ SMD RF IND
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TDK 13614
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AUD 0.0464
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded2 nH0.3 nH400 mA250 mOhms-- 55 C+ 125 C49.8 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLGReel , Cut Tape
MLG0603SR10JTD25


RF Inductors - SMD IND 0201 100nH StdQ AEC Q200 RF IND
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TDK 13612
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AUD 0.0587
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded100 nH5 %50 mA4.5 Ohms-- 55 C+ 125 C5940 MHzStandard0.6 mm0.3 mm0.3 mm-CeramicAEC - Q200MLGReel , Cut Tape
LQP03TN13NHZ2D


RF Inductors - SMD
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Murata 13580
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AUD 0.036
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded13 nH3 %250 mA800 mOhms-- 55 C+ 125 C122.6 GHzStandard0.6 mm0.3 mm0.3 mm-FerriteAEC - Q200LQPReel , Cut Tape
LQP02HQ6N8J02E


RF Inductors - SMD
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 13580
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AUD 0.0687
Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded6.8 nH5 %300 mA400 mOhms - 55 C+ 125 C135.7 GHzStandard0.4 mm0.2 mm0.3 mm Ferrite LQPReel , Cut Tape
LQW15AN22NG8ZD


RF Inductors - SMD 22 NH 2%
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Murata 13580
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AUD 0.1306
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded22 nH2 %780 mA202 mOhms-- 55 C+ 125 C4.54.5 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
NLCV32T-680K-EF


RF Inductors - SMD 68uH 3.64ohms 140mA Wound Ferrite
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TDK 13580
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AUD 0.1377
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded68 uH10 %140 mA2.8 Ohms-- 40 C+ 105 C1512 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFReel , Cut Tape
NLFV32T-330K-EF


RF Inductors - SMD 3.2mm x 2.5mm x 2.2mm, -40 to +105 degC, 95mA, 33?H, 780mohm
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TDK 13580
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AUD 0.1471
Multiples of: 2000

Wirewound1210 (3225 METRIC)Shielded33 uH10 %95 mA650 mOhms-- 40 C+ 105 C--Standard3.2 mm2.5 mm2.2 mm-Ferrite NLFV32 - EFReel , Cut Tape
MHQ1005P6N8JT000


RF Inductors - SMD IND 0402 6.8nH S-HQ SMD RF IND
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TDK 13475
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AUD 0.0965
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded6.8 nH5 %700 mA140 mOhms-- 55 C+ 125 C235.8 GHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
LQG15HN2N0S02D


RF Inductors - SMD 2 NH +-.3NH
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Murata 12804
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AUD 0.0095
Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded2 nH0.3 nH900 mA90 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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