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
  
                         
LQW18AN12NG00D


RF Inductors - SMD 12 NH 2%
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Murata 102102
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AUD 0.048
Multiples of: 20

Wirewound0603 (1608 METRIC)Unshielded12 nH2 %600 mA130 mOhms-- 55 C+ 125 C356 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
BSCH001608081N5S00


RF Inductors - SMD 1608 1.5nH
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Pulse 100860
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AUD 0.0505
Multiples of: 1

 1.6 mm x 0.8 mm x 0.8 mmShielded1.5 nH0.3 nH 100 mOhms600 mA- 55 C+ 125 C88 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic BSCHReel , Cut Tape
CIGT201610EH2R2MNE


RF Inductors - SMD CIGT,Thin Film,0806,2.2uH,1.0?,7 embossed,-20 20%
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Samsung 98502
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AUD 0.1386
Multiples of: 1

Thin Film Shielded2.2 uH20 %2.5 A74 mOhms2.7 A- 40 C+ 125 C--Standard2 mm1.6 mm1 mm-Metal Composite CIGTReel , Cut Tape
BSCH001608086N8J00


RF Inductors - SMD 1608 6.8nH
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Pulse 98358
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AUD 0.0505
Multiples of: 1

 1.6 mm x 0.8 mm x 0.8 mmShielded6.8 nH5 % 220 mOhms600 mA- 55 C+ 125 C103.75 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic BSCHReel , Cut Tape
PE-0402CL6N8JTT


RF Inductors - SMD 0402 6.8nH 300mA DCR=300mOhms RF
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Pulse 96966
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AUD 0.0315
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded6.8 nH5 %300 mA300 mOhms-- 55 C+ 125 C83.9 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
BSCH0016080812NJ00


RF Inductors - SMD 1608 12nH
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Pulse 96592
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AUD 0.0505
Multiples of: 1

 1.6 mm x 0.8 mm x 0.8 mmShielded12 nH5 % 280 mOhms600 mA- 55 C+ 125 C122.6 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic BSCHReel , Cut Tape
LQG15HN47NJ02D


RF Inductors - SMD Multi-Layer 47nH 5% 100MHz 8Q-Factor Air 200mA 1.15Ohm DCR 0402 Paper T/R
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Murata 95834
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AUD 0.0314
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded47 nH5 %250 mA1.15 Ohms-- 55 C+ 125 C81 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQP03TN1N0B02D


RF Inductors - SMD 1.0 NH
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Murata 93411
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AUD 0.0132
Multiples of: 50

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
BSCH001608081N0S00


RF Inductors - SMD 1nH RDC=0.10OhmS 600mA
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Pulse 93120
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AUD 0.0452
Multiples of: 4000

 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
LQG15HS18NJ02D


RF Inductors - SMD 18 NH 5%
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Murata 90792
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AUD 0.0219
Multiples of: 50

Multilayer0402 (1005 METRIC)Unshielded18 nH5 %400 mA360 mOhms-- 55 C+ 125 C82.2 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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