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
  
                         
LQG15HS1N0S02D


RF Inductors - SMD 1.0 NH +-.3NH
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Murata 120086
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AUD 0.011
Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded1 nH0.3 nH1 A70 mOhms-- 55 C+ 125 C810 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
ATFC-0402-3N5-BT


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.

ABRACON 119504
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AUD 0.0227
Multiples of: 5000

Thin Film Chip Inductor0402 (1005 METRIC)Unshielded3.5 nH0.1 nH380 mA550 mOhms - 45 C+ 85 C136 GHzStandard1 mm0.5 mm0.32 mm Ceramic ATFC - 0402Reel , Cut Tape
LQW2BAS39NJ00L


RF Inductors - SMD 39 NH 5%
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Murata 117913
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AUD 0.0948
Multiples of: 1

Wirewound0805 (2015 METRIC)Unshielded39 nH5 %500 mA290 mOhms-- 55 C+ 125 C602 GHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
BSCH000603033N0S00


RF Inductors - SMD 0603 3.0nH
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Pulse 116283
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AUD 0.0148
Multiples of: 1

 0.6 mm x 0.3 mm x 0.3 mmShielded3 nH0.3 nH 220 mOhms330 mA- 55 C+ 125 C47.2 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic BSCHReel , Cut Tape
LQG15WH36NG02D


RF Inductors - SMD Fixed IND 36nH 190mA POWRTRN
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Murata 114808
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AUD 0.1362
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded36 nH2 %190 mA1.5 Ohms-- 55 C+ 125 C201.6 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
PE-0402CL470JTT


RF Inductors - SMD 0402 47nH 200mA DCR=11000mOhms RF
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Pulse 113349
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AUD 0.0315
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded47 nH5 %200 mA1.1 Ohms-- 55 C+ 125 C81 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
CIGT201610UM1R0MNE


RF Inductors - SMD CIGT,Thin Film,0806,1.0uH,1.0?,7 embossed,-20 20%
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Samsung 113141
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AUD 0.1034
Multiples of: 1

Thin Film  1 uH20 %              CIGTReel , Cut Tape
LQG15HS27NJ02D


RF Inductors - SMD 27 NH 5%
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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 106312
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AUD 0.0116
Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded27 nH5 %350 mA460 mOhms - 55 C+ 125 C81.7 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQG15HS2N7S02D


RF Inductors - SMD 2.7 NH +-.3NH
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Murata 101365
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AUD 0.0112
Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded2.7 nH0.3 nH800 mA120 mOhms - 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQG15HZ39NJ02D


RF Inductors - SMD 39 NH .2%
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Murata 73733
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AUD 0.0397
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded39 nH5 %300 mA650 mOhms - 55 C+ 125 C81.2 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
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