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
  
                         
LQG15HS33NJ02D


RF Inductors - SMD 33 NH 5%
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Murata 112326
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AUD 0.0092
Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded33 nH5 %350 mA580 mOhms-- 55 C+ 125 C81.6 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
ASCH001005055N6SCP


RF Inductors - SMD 5.6nH RDC=0.20Ohms 400mA AEC-Q200
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Pulse 57774
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AUD 0.0362
Multiples of: 1

 1 mm x 0.5 mm x 0.5 mmShielded5.6 nH0.3 nH400 mA200 mOhms-- 55 C+ 125 C85.1 GHzStandard1 mm0.5 mm0.5 mm- AEC - Q200ASCHReel , Cut Tape
CIGT201210UHR47MNE


RF Inductors - SMD CIGT,Thin Film,0805,0.47uH,1.0?,7 embossed,-20 20%
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SAMSUNG 57064
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AUD 0.1155
Multiples of: 1

Thin Film Unshielded470 nH20 %3.6 A31 mOhms4.9 A- 40 C+ 125 C--Standard2 mm1.25 mm0.8 mm-  CIGTReel , Cut Tape
CIGT252010EH2R2MNE


RF Inductors - SMD CIGT,Thin Film,1008,2.2uH,1.0?,7 embossed,-20 20%
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Samsung 57002
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AUD 0.1737
Multiples of: 1

Thin Film Shielded2.2 uH20 %2.61 A77 mOhms2.5 A- 40 C+ 125 C--Standard2.5 mm2 mm1 mm-Metal Composite CIGTReel , Cut Tape
B82496C3820J


RF Inductors - SMD 82nH 220mA 5% 1.6x0.8mm SMD
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TDK 56834
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AUD 0.2072
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Wirewound0603 (1608 METRIC)Unshielded82 nH5 %220 mA1.5 Ohms-- 55 C+ 150 C142 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200SIMID - CReel , Cut Tape
LQP03TQ1N8C02D


RF Inductors - SMD 1.8nH 650mA 0201 (0603 metric) SUGGESTED ALT LQP03HQ1N8C02D
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Murata 56577
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AUD 0.0294
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded1.8 nH0.2 nH650 mA100 mOhms-- 55 C+ 125 C1715 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQW15AN6N0B80D


RF Inductors - SMD
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Murata 56127
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AUD 0.1064
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded6 nH0.1 nH1.6 A56 mOhms-- 55 C+ 125 C328 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
CIGT252010EH1R0MNE


RF Inductors - SMD CIGT,Thin Film,1008,1.0uH,1.0?,7 embossed,-20 20%
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SAMSUNG 55524
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AUD 0.1543
Multiples of: 1

Thin Film Unshielded1 uH20 %4.1 A30 mOhms4.7 A- 40 C+ 125 C--Standard2 mm1.25 mm0.8 mm-  CIGTReel , Cut Tape
CIGT201208TMR47MLE


RF Inductors - SMD 0.47uH, +/-20%, 0805, L Type, TH, in Film
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SAMSUNG 55354
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AUD 0.1657
Multiples of: 1

Wirewound0805 (2012 METRIC)Shielded470 nH20 %4.2 A24 mOhms4.8 A- 40 C+ 125 C  Standard2 mm1.2 mm0.8 mm Metal  Reel , Cut Tape
LQP03TN2N9B02D


RF Inductors - SMD 2.9 NH +-.1NH
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Murata 54902
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AUD 0.0041
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded2.9 nH0.1 nH500 mA200 mOhms - 55 C+ 125 C149.5 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
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