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
  
                         
CWF1610-150K


RF Inductors - SMD Ind,1.6x1x1mm,15uH+/-10%,0.24A,non-shd
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Bourns 5988
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AUD 0.1413
Multiples of: 1

Wirewound0603 (1610 METRIC)Semi - Shielded15 uH10 %240 mA -- 40 C+ 125 C--Standard1.6 mm1 mm1 mm-Ferrite CWF1610Reel , Cut Tape
MHQ1005075HA2N1BTD25


RF Inductors - SMD FIXED IND 2.1NH 1A 50 MOHM SMD
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TDK 5982
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AUD 0.1147
Multiples of: 1

Multilayer Ceramic Inductor0402 (1005 METRIC)Shielded2.1 nH0.1 nH1 A50 mOhms - 55 C+ 125 C2013.6 GHzStandard1 mm0.5 mm0.7 mm Ceramic MHQReel , Cut Tape
MLJ1005WR12JT000


RF Inductors - SMD 0402 120nH 5% 0.39ohm 380mA
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TDK 5981
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AUD 0.1419
Multiples of: 1

NFC Inductor0402 (1005 METRIC)Shielded120 nH5 %450 mA390 mOhms450 mA- 55 C+ 125 C15740 MHzStandard1 mm0.5 mm0.5 mm-Ferrite MLJReel , Cut Tape
MLF1005VR12JTD25


RF Inductors - SMD 0402 0.12uH 5% AEC-Q200
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TDK 5979
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AUD 0.0247
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Multilayer0402 (1005 METRIC)Shielded120 nH5 %180 mA590 mOhms-- 55 C+ 125 C10800 MHzStandard1 mm0.5 mm0.5 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQW18AN3N6D0ZD


RF Inductors - SMD
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Murata 5977
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AUD 0.1293
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded3.6 nH0.5 nH850 mA59 mOhms-- 55 C+ 125 C256 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
LQW15AN4N8B80D


RF Inductors - SMD
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Murata 5973
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AUD 0.1053
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded4.8 nH0.1 nH1.2 A71 mOhms-- 55 C+ 125 C308 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQW15AN8N4G80D


RF Inductors - SMD
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Murata 5964
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AUD 0.134
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded8.4 nH2 %1.5 A69 mOhms-- 55 C+ 125 C326.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
MLF1608A1R5JTD25


RF Inductors - SMD 1.5uH 700mohms 50mA +/-5% Fer AEC-Q200
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TDK 5917
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AUD 0.1586
Multiples of: 1

Multilayer0603 (1608 METRIC)Shielded1.5 uH5 %50 mA700 mOhms-- 55 C+ 125 C35140 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
MLG0603P2N0ST000


RF Inductors - SMD IND 0201 2.0nH Hi-Q SMD RF IND
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TDK 5917
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AUD 0.0038
Multiples of: 100

Multilayer0201 (0603 METRIC)Unshielded2 nH0.3 nH600 mA100 mOhms-- 55 C+ 125 C1410.1 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic MLG - PReel , Cut Tape
LQG15HN47NH02D


RF Inductors - SMD
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Murata 5480
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AUD 0.0228
Multiples of: 50

Multilayer0402 (1005 METRIC)Unshielded47 nH3 %250 mA1.15 Ohms-- 55 C+ 125 C81 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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