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
  
                         
BSCH001608081N0S00


RF Inductors - SMD 1nH RDC=0.10OhmS 600mA
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Pulse 92201
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AUD 0.041
Multiples of: 1

 1.6 mm x 0.8 mm x 0.8 mmShielded1 nH0.3 nH 100 mOhms600 mA- 55 C+ 125 C810 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic BSCHReel , Cut Tape
CIGT201610LH2R2MNE


RF Inductors - SMD CIGT,Thin Film,0806,2.2uH,1.0?,7 embossed,-20 20%
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Samsung 85329
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AUD 0.1232
Multiples of: 1

Thin Film Shielded2.2 uH20 %1.8 A139 mOhms2 A- 40 C+ 125 C--Standard2 mm1.6 mm1 mm-Metal Composite CIGTReel , Cut Tape
LQP03TN68NJ02D


RF Inductors - SMD 68 NH 5%
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Murata 84584
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AUD 0.004
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded68 nH5 %100 mA8 Ohms-- 55 C+ 125 C81.1 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
PE-0402CL3N9STT


RF Inductors - SMD 0402 3.9nH 300mA DCR=200mOhms RF
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Pulse 84448
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AUD 0.0315
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded3.9 nH0.3 nH300 mA200 mOhms-- 55 C+ 125 C84 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
BSCH0016080815NJ00


RF Inductors - SMD 15nH RDC=0.32Ohms 600mA
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Pulse 80235
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AUD 0.0485
Multiples of: 1

 1.6 mm x 0.8 mm x 0.8 mmShielded15 nH5 % 320 mOhms600 mA- 55 C+ 125 C122.5 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic BSCHReel , Cut Tape
LQW15AN36NG80D


RF Inductors - SMD 36 NH 2%
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Murata 80226
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AUD 0.1155
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded36 nH2 %540 mA309 mOhms-- 55 C+ 125 C303.8 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQP03TG3N3C02D


RF Inductors - SMD
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 79769
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between Tue. 17 Feb to Thu. 19 Feb Calender.png

AUD 0.0151
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
CIGT160808XMR24MNC


RF Inductors - SMD CIGT,Thin Film,0603,0.24uH,0.8?,7 paper,-20 20%
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SAMSUNG 79642
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AUD 0.139
Multiples of: 1

Thin Film  240 nH20 %              CIGTReel , Cut Tape
AISC-0402-15NJ-T


15 nH Unshielded Drum Core, Wirewound Inductor 560 mA 170mOhm Max 0402 (1005 Metric)
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ABRACON 79171
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AUD 0.1675
Multiples of: 2500

Ceramic Wirewound RF Inductor0402 (1005 METRIC)Unshielded15 nH5 %560 mA170 mOhms   263.28 GHzStandard1.1 mm0.6 mm0.66 mm Ceramic AISC - 0402Reel , Cut Tape
LQG15HS27NJ02D


RF Inductors - SMD 27 NH 5%
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 74884
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AUD 0.0066
Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded27 nH5 %350 mA460 mOhms - 55 C+ 125 C81.7 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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