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
  
                         
MLG1005S8N2JT000


RF Inductors - SMD IND 0402 8.2nH StdQ SMD RF IND
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TDK 19145
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AUD 0.0678
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded8.2 nH5 %500 mA300 mOhms-- 55 C+ 125 C84 GHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , 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
Multiples of: 1

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
Multiples of: 1

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
MLF1608DR56JTD25


RF Inductors - SMD 560nH 1.05ohms 100mA +/-5% Fer AEC-Q200
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TDK 19126
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AUD 0.155
Multiples of: 1

Multilayer0603 (1608 METRIC)Shielded560 nH5 %100 mA1.05 Ohms-- 55 C+ 125 C15230 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQP02TN0N7B02D


RF Inductors - SMD
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Murata 19109
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AUD 0.0101
Multiples of: 50

Thin Film01005 (0402 METRIC)Unshielded700 pH0.1 nH320 mA500 mOhms - 55 C+ 125 C816.5 GHzStandard0.4 mm0.2 mm0.2 mm Ferrite LQPReel , 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
Multiples of: 1

 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
LQG15HN9N1G02D


RF Inductors - SMD 9.1 NH +-2%
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Murata 19109
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AUD 0.0455
Multiples of: 1

Multilayer Unshielded9.1 nH30 %500 mA270 mOhms-- 55 C+ 125 C83.4 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQP02TN0N9B02D


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 19109
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between Thu. 19 Feb to Mon. 23 Feb Calender.png

AUD 0.0459
Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded900 pH0.1 nH320 mA500 mOhms - 55 C+ 125 C813 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
LQP02TQ17NH02D


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 19109
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between Thu. 19 Feb to Mon. 23 Feb Calender.png

AUD 0.103
Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded17 nH3 %140 mA2.5 Ohms-- 55 C+ 125 C102.5 GHzStandard0.4 mm0.2 mm0.2 mm-Ferrite LQPReel , Cut Tape
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