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
  
                         
CIGT201610LHR24MNE


RF Inductors - SMD CIGT,Thin Film,0806,0.24uH,1.0?,7 embossed,-20 20%
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SAMSUNG 69318
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AUD 0.1224
Multiples of: 1

Thin Film  240 nH20 %              CIGTReel , Cut Tape
PE-0402CL2N0STT


RF Inductors - SMD 0402 2nH 300mA DCR=200mOhms RF
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Pulse 68912
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AUD 0.0276
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded2 nH0.3 nH300 mA200 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
AIAC-4125C-R206J-T


RF Inductors - SMD FIXED IND 206NH 3A 10.5 MOHM SMD
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ABRACON 68672
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AUD 0.6253
Multiples of: 1000

SMT Air Coil Inductor9 mm x 4.4 mm x 4.6 mmUnshielded206 nH5 %3 A10.5 mOhms - 40 C+ 125 C100700 MHzStandard9 mm4.4 mm4.6 mm Air AIAC - 4125CReel , Cut Tape
B82496C3120J


RF Inductors - SMD 12nH 450mA 5% 1.6x0.8mm SMD
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TDK 67989
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AUD 0.2204
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded12 nH5 %450 mA350 mOhms-- 55 C+ 150 C145 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200SIMID - CReel , Cut Tape
ASCH0010050512NJCP


RF Inductors - SMD Chilisin RF inductor Multilayer-STD
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Pulse 67900
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AUD 0.041
Multiples of: 1

 1 mm x 0.5 mm x 0.5 mmShielded12 nH5 %300 mA280 mOhms - 55 C+ 125 C83 GHzStandard1 mm0.5 mm0.5 mm  AEC - Q200ASCHReel , Cut Tape
B82422A1223K100


RF Inductors - SMD 22uH 140mA 10% 1210 SMD, AEC-Q200
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TDK 65628
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AUD 0.2068
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded22 uH10 %140 mA2.65 Ohms-- 55 C+ 145 C2716 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
LQP03TG3N3C02D


RF Inductors - SMD
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Murata 64205
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AUD 0.0138
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded3.3 nH0.2 nH400 mA320 mOhms - 55 C+ 125 C139.5 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
ASCH001005056N8JCP


RF Inductors - SMD 1005 6.8nH AEC-Q200
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Pulse 63040
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AUD 0.0345
Multiples of: 1

 1 mm x 0.5 mm x 0.5 mmShielded6.8 nH5 %400 mA240 mOhms-- 55 C+ 125 C84.55 GHzStandard1 mm0.5 mm0.5 mm- AEC - Q200ASCHReel , Cut Tape
LQW18ASR10G0ZD


RF Inductors - SMD 100 NH 2%
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Murata 59003
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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
LQW15AN9N0G00D


9nH SMD,0.5x1mm Inductors (SMD) ROHS
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Murata 9700
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AUD 0.0489
Multiples of: 10

Wirewound0402 (1005 METRIC)Unshielded9 nH2 %540 mA140 mOhms-- 55 C+ 125 C255.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
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