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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Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
MHQ0603P2N0BT000


RF Inductors - SMD IND 0201 2.0nH S-HQ SMD RF IND
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TDK 14475
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between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.0495

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded2 nH0.1 nH700 mA120 mOhms-- 55 C+ 125 C1613.8 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
MLG0603S6N8JT000


RF Inductors - SMD IND 0201 6.8nH StdQ SMD RF IND
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TDK 14472
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between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.0372

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded6.8 nH5 %250 mA600 mOhms-- 55 C+ 125 C54.4 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLGReel , Cut Tape
MLG0603SR18JTD25


RF Inductors - SMD IND 0201 180nH StdQ AEC Q200 RF IND
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TDK 14472
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between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.0727

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Multilayer0201 (0603 METRIC)Unshielded180 nH5 %50 mA8.5 Ohms-- 55 C+ 125 C5680 MHzStandard0.6 mm0.3 mm0.3 mm-CeramicAEC - Q200MLGReel , Cut Tape
MHQ0603P5N1CT000


RF Inductors - SMD IND 0201 5.1nH S-HQ SMD RF IND
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TDK 14469
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AUD 0.0422

Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded5.1 nH0.2 nH350 mA400 mOhms-- 55 C+ 125 C167.8 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
BSPQ000603044N0B00


RF Inductors - SMD 4nH 500MHz 500mA RDC=0.17mOhms
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Pulse 14466
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AUD 0.0757

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 0.6 mm x 0.3 mm x 0.4 mmShielded4 nH0.1 nH500 mA170 mOhms500 mA- 55 C+ 125 C207 GHzStandard0.6 mm0.3 mm0.4 mm Ceramic BSPQReel , Cut Tape
BSPQ000603049N1H00


RF Inductors - SMD 9.1nH 500MHz 300mA RDC=0.40mOhms
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Pulse 14462
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between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.0702

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 0.6 mm x 0.3 mm x 0.4 mmShielded9.1 nH3 %300 mA400 mOhms300 mA- 55 C+ 125 C204.5 GHzStandard0.6 mm0.3 mm0.4 mm Ceramic BSPQReel , Cut Tape
PE-0805CD221JTT


RF Inductors - SMD SMD IND
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Pulse 14462
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between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.2072

Multiples of: 1

Multilayer0805 (2012 METRIC)Unshielded217 nH5 %400 mA700 mOhms-- 40 C+ 125 C45850 MHzStandard2.29 mm1.68 mm1.58 mm-Ceramic CDReel , Cut Tape
BSPQ000603043N0B00


RF Inductors - SMD 3nH 500MHz 600mA RDC=0.12mOhms
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Pulse 14461
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between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.0702

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 0.6 mm x 0.3 mm x 0.4 mmShielded3 nH0.1 nH600 mA120 mOhms600 mA- 55 C+ 125 C208 GHzStandard0.6 mm0.3 mm0.4 mm Ceramic BSPQReel , Cut Tape
LQP03TN3N2C02D


RF Inductors - SMD
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Murata 14457
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between Fri. 21 Nov to Tue. 25 Nov
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AUD 0.0186

Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded3.2 nH0.2 nH450 mA250 mOhms-- 55 C+ 125 C148 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP03TN18NH02D


RF Inductors - SMD 18 NH
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Murata 14453
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between Mon. 01 Dec to Thu. 04 Dec
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AUD 0.0063

Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded18 nH3 %200 mA800 mOhms-- 55 C+ 125 C122.2 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
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