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
  
                         
LQG15HS27NJ02D


RF Inductors - SMD 27 NH 5%
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Murata 58200
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AUD 0.0278
Multiples of: 10000

Multilayer0402 (1005 METRIC)Unshielded27 nH5 %350 mA460 mOhms - 55 C+ 125 C81.7 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQW2BAS24NG00L


RF Inductors - SMD
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Murata 45917
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AUD 0.1535
Multiples of: 1

Wirewound Unshielded24 nH2 %500 mA220 mOhms-- 55 C+ 125 C502.4 GHzStandard2.09 mm1.53 mm1.42 mm-Ferrite LQW2BAReel , Cut Tape
PE-0402CL2N2STT


RF Inductors - SMD 0402 2.2nH 300mA DCR=200mOhms RF
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Pulse 45722
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AUD 0.0264
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded2.2 nH0.3 nH300 mA200 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
LQG15WZ33NG02D


RF Inductors - SMD 33 NH 2%
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Murata 45236
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AUD 0.1238
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded33 nH2 %220 mA1.5 Ohms-- 55 C+ 125 C201.6 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
B82422-A1103-K100


RF Inductors - SMD 10uH 180mA 10% 1210 SMD, AEC-Q200
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TDK 44650
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AUD 0.2475
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded10 uH10 %180 mA1.6 Ohms-- 55 C+ 145 C2725 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
CIGT160808XMR24MNC


RF Inductors - SMD CIGT,Thin Film,0603,0.24uH,0.8?,7 paper,-20 20%
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SAMSUNG 41728
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AUD 0.132
Multiples of: 1

Thin Film  240 nH20 %              CIGTReel , Cut Tape
LQG15HS1N2B02D


1A 1.2nH 70mO 0402 Inductors (SMD) ROHS
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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 40851
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AUD 0.0396
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded1.2 nH0.1 nH1 A70 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQP03TN4N7H02D


RF Inductors - SMD 4.7 NH
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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 36084
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AUD 0.0131
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded4.7 nH3 %350 mA400 mOhms-- 55 C+ 125 C144.4 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP03HQ4N7H02D


RF Inductors - SMD 4.7 NH 3%
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Murata 32029
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AUD 0.0346
Multiples of: 20

Thin Film0201 (0603 METRIC)Unshielded4.7 nH3 %400 mA250 mOhms - 55 C+ 125 C207 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
MLF1608C220KTA00


Inductor RF Chip Shielded Multi-Layer 22uH 10% 1MHz 20Q-Factor Ferrite 2mA 1.7Ohm DCR 0603 T/R
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TDK 3967
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AUD 0.0544
Multiples of: 10

Multilayer0603 (1608 METRIC)Shielded22 uH10 %2 mA1.7 Ohms-- 55 C+ 125 C2038 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
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