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
  
                         
ISC1812ES150K


RF Inductors - SMD 15uh 10%
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Vishay 1940
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AUD 0.7848
Multiples of: 1

Molded1812 (4532 METRIC)    15 mOhms     Standard      ISCReel , Cut Tape
PM105SB-151K-RC


Inductor Power Shielded Bobbin Core 150uH 10% 100KHz 24Q-Factor Ferrite 550mA 510mOhm DCR T/R
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Bourns 1940
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AUD 0.8112
Multiples of: 500

Wirewound Shielded150 uH10 %550 mA510 mOhms-- 30 C+ 100 C246 MHzStandard4.5 mm--9.9 mmFerrite PM105SBReel , Cut Tape
ISC1812ER100J


RF Inductors - SMD 10uh 5%
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Vishay 1940
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AUD 0.8437
Multiples of: 1

Molded1812 (4532 METRIC) 10 uH  820 mOhms     Standard      ISCReel , Cut Tape
1210-332J


RF Inductors - SMD 3.3uH 5%
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Delevan 1940
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AUD 2.0571
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded3.3 uH5 %393 mA1.2 Ohms-- 55 C+ 125 C3058 MHzStandard3.51 mm2.67 mm2.57 mm-  1210/RReel , Cut Tape
AISC-1008-R47G-T


RF Inductors - SMD FIXED IND 470NH 470MA 1.19 OHM
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ABRACON 1939
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AUD 0.2952
Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded470 nH2 %470 mA1.19 Ohms - 40 C+ 125 C50450 MHzStandard2.92 mm2.79 mm2.29 mm Ceramic AISC - 1008Reel , Cut Tape
CMH322522-820KL


RF Inductors - SMD 82uH 10% 2.52MHz
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Bourns 1939
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AUD 0.418
Multiples of: 1

Wirewound1210 (3225 METRIC)Shielded82 uH10 %45 mA10 Ohms-- 55 C+ 125 C3010 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite  Reel , Cut Tape
IWC1008DR68R-3G


RF Inductors - SMD 1008 680nH 2% 400mA
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Laird Performance Materials 1938
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AUD 0.1898
Multiples of: 1

Wirewound2.92 mm x 2.7 mm x 2.33 mmUnshielded680 nH2 %400 mA1.47 Ohms-- 40 C+ 125 C45375 MHzStandard2.92 mm2.7 mm2.33 mm-Ceramic IWC1008Reel , Cut Tape
PM1008-5R6K-RC


RF Inductors - SMD 5.6uH 10%
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Bourns 1938
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AUD 0.2172
Multiples of: 1

 1008 (2520 METRIC)Unshielded5.6 uH10 %180 mA7 Ohms   2055 MHzStandard2.5 mm2 mm1.6 mm   PM1008Reel , Cut Tape
1206F-100K-01


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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Fastron 1937
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AUD 0.3352
Multiples of: 1

Wirewound1206 (3216 METRIC)Unshielded10 uH10 %200 mA4 Ohms-- 40 C+ 100 C25100 MHzStandard4 mm2.5 mm1.6 mm-FerriteAEC - Q2001206FReel , Cut Tape
PM105-101K-RC


Inductor Power Bobbin Core 100uH 10% 1KHz 15Q-Factor Ferrite 970mA 350mOhm DCR T/R
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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.

Bourns 1716
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AUD 1.0438
Multiples of: 500

Wirewound Unshielded100 uH10 %970 mA350 mOhms1.7 A- 30 C+ 100 C297 MHzStandard5.8 mm--9.8 mmFerrite PM105Reel , Cut Tape
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