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
  
                         
LQP03TN15NHZ2D


RF Inductors - SMD 15 NH 3%
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Murata 21407
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AUD 0.0362
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded15 nH3 %250 mA700 mOhms-- 55 C+ 125 C122.6 GHzStandard0.6 mm0.3 mm0.3 mm-FerriteAEC - Q200LQPReel , Cut Tape
NLV25T-1R5J-EF


RF Inductors - SMD 1.5uH 1.3ohms 220mA Wound Ferrite
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TDK 3880
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AUD 0.1303
Multiples of: 2000

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded1.5 uH5 %220 mA1.3 Ohms-- 40 C+ 105 C30182 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
MIL8532-16L


RF Inductors - SMD M27/370-16, Surface Mount, High Current, MIL-PRF-27/370 Qualified Power Inductors, 18 uH , +/- 15%
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Delevan 81
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AUD 7.5194
Multiples of: 1

Established Reliability Unshielded18 uH15 %2.84 A44 mOhms - 55 C+ 130 C  Standard22.35 mm8.38 mm7.26 mm Ferrite MIL8532Reel , Cut Tape
LBM2016T5R6J


RF Inductors - SMD 963-LSQMB201616T5R6J RPLCMT PN 0806 5.6uH 1144mOhms 5% 255mA
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Taiyo Yuden 80
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AUD 0.0914
Multiples of: 1

Wirewound0806 (2016 METRIC)Unshielded5.6 uH5 %255 mA1.14 Ohms-- 40 C+ 105 C2536 MHzStandard2 mm1.6 mm1.8 mm-  LBMReel , Cut Tape
LQW18AN27NG10D


RF Inductors - SMD 27 NH 2%
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Murata 77
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AUD 0.0542
Multiples of: 10

Wirewound0603 (1608 METRIC)Unshielded27 nH2 %590 mA116 mOhms-- 55 C+ 125 C422.8 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
2222SQ-271GEC


RF Inductors - SMD 2222 270nH Unshld 2% 4.3A 12.5mOhms
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Coilcraft 77
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AUD 1.7799
Multiples of: 1

Wirewound5.59 mm x 5.69 mm x 11.68 mmUnshielded270 nH2 %4.3 A12.5 mOhms-- 40 C+ 125 C140800 MHzStandard11.68 mm5.59 mm5.69 mm-Air 2222SQReel , Cut Tape
S1210-822J


RF Inductors - SMD 8.2uH 5% 1.7ohm Shielded SMT Induc
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Delevan 76
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AUD 3.3
Multiples of: 1

Wirewound1210 (3225 METRIC)Shielded8.2 uH5 %308 mA1.7 Ohms-- 55 C+ 125 C4032 MHzStandard3.51 mm2.66 mm2.57 mm-Ferrite S1210/RReel , Cut Tape
5022-621J


RF Inductors - SMD 0.62 uH 5%
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Delevan 76
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AUD 5.5657
Multiples of: 1

Filter Choke Unshielded620 nH5 %1.62 A140 mOhms-- 55 C+ 125 C50260 MHzStandard13.21 mm6.35 mm5.84 mm-Phenolic 5022Reel , Cut Tape
LQG15HZ33NH02D


RF Inductors - SMD
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Murata 58
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AUD 0.0278
Multiples of: 20

Multilayer0402 (1005 METRIC)Unshielded33 nH3 %350 mA580 mOhms - 55 C+ 125 C81.6 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
1210F-470K-01


RF Inductors - SMD Wire-wound Ferrite RF Chip Inductor
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Fastron 0
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AUD 0.3197
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded47 uH10 %210 mA2.3 Ohms-- 40 C+ 100 C256.5 MHzStandard3.8 mm3 mm2.4 mm-FerriteAEC - Q2001210FReel , Cut Tape
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