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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Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
PM1008-100K-RC


RF Inductors - SMD 10uH 10%
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Bourns 1543
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.2442

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded10 uH10 %200 mA12 Ohms-- 55 C+ 125 C2025 MHzStandard2.5 mm2 mm1.6 mm-Ferrite PM1008Reel , Cut Tape
LQP03TN5N1J02D


RF Inductors - SMD
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Murata 1542
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.0208

Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded5.1 nH5 %350 mA400 mOhms-- 55 C+ 125 C144.2 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
NLFV25T-1R5M-EF


RF Inductors - SMD 1.5uH 110mohms 350mA Wound Ferrite
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TDK 1539
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1553

Multiples of: 1

Wirewound2.5 mm x 2 mm x 1.8 mmShielded1.5 uH20 %350 mA90 mOhms-- 40 C+ 105 C--Standard2.5 mm2 mm1.8 mm-Ferrite NLFV25 - EFReel , Cut Tape
NLV32T-121J-EFD


RF Inductors - SMD 120uH 11ohms 70mA Wound Fer AEC-Q200
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TDK 1538
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between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.0659

Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded120 uH5 %70 mA11 Ohms-- 40 C+ 105 C2010 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
1008AS-R12J-01


RF Inductors - SMD 120nH 25 MHz 5% Tol
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Fastron 1529
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.204

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded120 nH5 %650 mA630 mOhms-- 40 C+ 125 C60950 MHzStandard2.9 mm2.8 mm2.1 mm-CeramicAEC - Q2001008ASReel , Cut Tape
S1812R-124K


RF Inductors - SMD 120uH 10%
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API Delevan 1527
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between Mon. 01 Dec to Wed. 03 Dec
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AUD 3.9577

Multiples of: 1

RF Choke1812 (4532 METRIC)Shielded120 uH10 %163 mA7.5 Ohms-- 55 C+ 125 C406 MHzStandard4.8 mm3.4 mm3.4 mm-Ferrite S1812/RReel , Cut Tape
MLF1608DR68JT000


RF Inductors - SMD .68 UH 5%
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TDK 1493
Ships to you
between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.0459

Multiples of: 20

Multilayer0603 (1608 METRIC)Shielded680 nH5 %70 mA1.25 Ohms-- 55 C+ 125 C15210 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLFReel , Cut Tape
NLCV32T-150K-EF


RF Inductors - SMD 15uH 728mohms 370mA Wound Ferrite
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TDK 1358
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between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.061

Multiples of: 10

Wirewound1210 (3225 METRIC)Unshielded15 uH10 %370 mA560 mOhms-- 40 C+ 105 C1526 MHzStandard3.2 mm2.5 mm2.4 mm-Ferrite NLCV - EFReel , Cut Tape
NLV25T-100J-PF


RF Inductors - SMD SUGGESTED ALTERNATE NLV25T-100J-EF
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TDK 1338
Ships to you
between Tue. 09 Dec to Fri. 12 Dec
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AUD 0.052

Multiples of: 10

Wirewound Unshielded10 uH5 %155 mA3.5 Ohms-- 40 C+ 105 C2533 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - PFReel , Cut Tape
LQW2UASR33J00L


RF Inductors - SMD .33 UH 5%
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Murata 253
Ships to you
between Mon. 01 Dec to Wed. 03 Dec
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AUD 0.1411

Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded330 nH5 %450 mA1.05 Ohms-- 55 C+ 125 C45570 MHzStandard2.62 mm2.45 mm1.83 mm-Air LQWReel , Cut Tape
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