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
  
                         
MHQ0603P2N1BTD25


RF Inductors - SMD 0201 2.1nH Tol 0.1nH AEC-Q200
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TDK 11858
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AUD 0.0776
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded2.1 nH0.1 nH700 mA150 mOhms-- 55 C+ 125 C1612.7 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
LQP03TN4N1B02D


RF Inductors - SMD 4.1 NH +/-0.1NH
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Murata 11785
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AUD 0.0085
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
LQP02TN1N6B02D


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 11785
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AUD 0.0131
Multiples of: 50

Thin Film01005 (0402 METRIC)Unshielded1.6 nH0.1 nH220 mA600 mOhms - 55 C+ 125 C89.5 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
LCCI0603S4N7GTAR


RF Inductors - SMD 4.7nH Tol 0.3nH 0603 1000mA DCR=0.2 Ohms
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Kyocera AVX 11769
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AUD 0.0291
Multiples of: 1

Multilayer0603 (1608 METRIC)Unshielded4.7 nH0.3 nH1 A200 mOhms-- 40 C+ 85 C105 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic LCCIReel , Cut Tape
LQG15WH72NG02D


RF Inductors - SMD Fixed IND 72nH 160mA POWRTRN
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Murata 11742
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AUD 0.1449
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded72 nH2 %160 mA2.2 Ohms-- 55 C+ 125 C221.1 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
MHQ0402PSA12NHT000


RF Inductors - SMD 01005, 12nH +-3% S-HQ SMD RF IND
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TDK 11735
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AUD 0.0234
Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded12 nH3 %130 mA1.9 Ohms-- 55 C+ 125 C84.8 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQW15AN5N3B80D


RF Inductors - SMD 5.3 NH +-.1NH
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Murata 11732
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AUD 0.1228
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded5.3 nH0.1 nH1.77 A40 mOhms-- 55 C+ 125 C358 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
MLF1005VR10KT000


RF Inductors - SMD 1mm x 0.5mm x 0.5mm, -55 to +125 degC, 180mA, 0.1?H, 510mohm
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TDK 11719
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AUD 0.1514
Multiples of: 1

Multilayer0402 (1005 METRIC)Shielded100 nH10 %180 mA510 mOhms-- 55 C+ 125 C10880 MHzStandard1 mm0.5 mm0.5 mm-Ferrite MLFReel , Cut Tape
MLG1005S3N0BT000


RF Inductors - SMD IND 0402 3.0nH StdQ SMD RF IND
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TDK 11707
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AUD 0.0076
Multiples of: 10

Multilayer0402 (1005 METRIC)Unshielded3 nH0.1 nH800 mA200 mOhms-- 55 C+ 125 C76.8 GHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , Cut Tape
LQP03TG1N6B02D


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 11543
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AUD 0.004
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded1.6 nH0.1 nH600 mA150 mOhms - 55 C+ 125 C1313 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
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