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
  
                         
BWCS00231715R47G00


RF Inductors - SMD 470nH RDC=1.76Ohms 250mA
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Pulse 34861
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AUD 0.101
Multiples of: 1

 2.35 mm x 1.73 mm x 1.52 mmUnshielded470 nH2 %250 mA1.76 Ohms250 mA- 40 C+ 125 C33450 MHzStandard2.35 mm1.73 mm1.52 mm Ceramic BWCSReel , Cut Tape
B82422H1334K


RF Inductors - SMD 330uH 90mA 10% 3.2x2.5mm SMD
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TDK 34546
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AUD 0.3718
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded330 uH10 %90 mA14 Ohms115 mA- 55 C+ 150 C154.5 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200B82422HReel , Cut Tape
LQP02HQ2N5W02L


RF Inductors - SMD
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Murata 34033
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AUD 0.1171
Multiples of: 1

Thin Film Unshielded2.5 nH0.05 nH450 mA200 mOhms-- 55 C+ 125 C1411 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQW18AN72NG00D


RF Inductors - SMD 72 NH 2%
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Murata 33969
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AUD 0.0381
Multiples of: 20

Wirewound0603 (1608 METRIC)Unshielded72 nH2 %270 mA560 mOhms-- 55 C+ 125 C342.1 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
MLF1608DR10KTA00


RF Inductors - SMD 1.6mm x 0.8mm x 0.8mm, -55 to +125 degC, 200mA, 0.1?H, 350mohm
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TDK 33759
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AUD 0.0811
Multiples of: 1

Multilayer0603 (1608 METRIC)Shielded100 nH10 %200 mA350 mOhms-- 55 C+ 125 C15600 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
36502AR82JTDG


RF Inductors - SMD 3650 2A 0.82uH 5% 2K RL
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TE Connectivity 33672
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AUD 0.3086
Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded820 nH5 %180 mA2.35 Ohms-- 40 C+ 125 C23200 MHzStandard2.29 mm1.73 mm1.52 mm-  3650Reel , Cut Tape
LQW18ANR10G00D


RF Inductors - SMD .1 UH 2%
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Murata 33610
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AUD 0.0394
Multiples of: 10

Wirewound0603 (1608 METRIC)Unshielded100 nH2 %220 mA680 mOhms-- 55 C+ 125 C341.8 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQP03TN4N3H02D


RF Inductors - SMD 4.3 NH
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Murata 33562
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AUD 0.0038
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded4.3 nH3 %350 mA400 mOhms-- 55 C+ 125 C145.3 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP03TN1N5BZ2D


RF Inductors - SMD
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Murata 33432
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AUD 0.0379
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded1.5 nH0.1 nH600 mA150 mOhms-- 55 C+ 125 C1415 GHzStandard0.6 mm0.3 mm0.3 mm-FerriteAEC - Q200LQPReel , Cut Tape
LQW18ASR10G0ZD


RF Inductors - SMD 100 NH 2%
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Murata 26070
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AUD 0.1051
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded100 nH2 %400 mA580 mOhms-- 40 C+ 125 C341.4 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
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