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
  
                         
LQW2BAS39NJ00L


RF Inductors - SMD 39 NH 5%
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Murata 129375
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AUD 0.1082
Multiples of: 1

Wirewound0805 (2015 METRIC)Unshielded39 nH5 %500 mA290 mOhms-- 55 C+ 125 C602 GHzStandard2.09 mm1.53 mm1.42 mm-Air LQW2BAReel , Cut Tape
LQW15AN2N6G8ZD


RF Inductors - SMD
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Murata 126950
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AUD 0.1323
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded2.6 nH2 %1.95 A35 mOhms-- 55 C+ 125 C3014.5 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
BSCH000603038N2J00


RF Inductors - SMD 0603 8.2nH
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Pulse 124111
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AUD 0.0175
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 0.6 mm x 0.3 mm x 0.3 mmShielded8.2 nH5 % 450 mOhms230 mA- 55 C+ 125 C43.4 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic BSCHReel , Cut Tape
LQW15AN33NJ80D


RF Inductors - SMD 33 NH 5%
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Murata 120311
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AUD 0.099
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Wirewound0402 (1005 METRIC)Unshielded33 nH5 %620 mA336 mOhms-- 55 C+ 125 C303.6 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
BSCH000603033N0S00


RF Inductors - SMD 0603 3.0nH
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Pulse 116293
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AUD 0.0152
Multiples of: 1

 0.6 mm x 0.3 mm x 0.3 mmShielded3 nH0.3 nH 220 mOhms330 mA- 55 C+ 125 C47.2 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic BSCHReel , Cut Tape
PE-0402CL470JTT


RF Inductors - SMD 0402 47nH 200mA DCR=11000mOhms RF
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Pulse 113349
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AUD 0.0315
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded47 nH5 %200 mA1.1 Ohms-- 55 C+ 125 C81 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
CI160808-22NJ


RF Inductors - SMD 22nH 5% MultiLayer High Frequency
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Bourns 108640
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AUD 0.0446
Multiples of: 4000

Multilayer0603 (1608 METRIC)Unshielded22 nH5 %300 mA550 mOhms-- 55 C+ 125 C101.1 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic CI160808Reel , Cut Tape
LQP03TN1N0B02D


RF Inductors - SMD 1.0 NH
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Murata 94187
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AUD 0.0041
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded1 nH0.1 nH750 mA100 mOhms - 55 C+ 125 C1417 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQG15HS15NJ02D


RF Inductors - SMD 15 NH 5%
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Murata 61595
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AUD 0.0079
Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded15 nH5 %450 mA320 mOhms-- 55 C+ 125 C82.5 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
CIGT201208EHR47MNE


RF Inductors - SMD CIGT,Thin Film,0805,0.47uH,0.8?,7 embossed,-20 20%
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SAMSUNG 0
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AUD 0.1449
Multiples of: 1

Thin Film Unshielded470 nH20 %4.1 A35 mOhms4.3 A- 40 C+ 125 C--Standard2 mm1.25 mm0.8 mm-  CIGTReel , Cut Tape
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