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
  
                         
LQW15AN9N5J00D


RF Inductors - SMD 9.5 NH 5%
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Murata 10534
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AUD 0.0495
Multiples of: 20

Wirewound0402 (1005 METRIC)Unshielded9.5 nH5 %540 mA140 mOhms-- 55 C+ 125 C255.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
MHQ1005075HA6N8JTD25


RF Inductors - SMD FIXED IND 6.8NH 0.5A 200 MOHM SMD
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TDK 863
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AUD 0.11
Multiples of: 1

Multilayer Ceramic Inductor0402 (1005 METRIC)Shielded6.8 nH5 %500 mA200 mOhms - 55 C+ 125 C205.5 GHzStandard1 mm0.5 mm0.7 mm Ceramic MHQReel , Cut Tape
MHQ1005075HA7N3JTD25


RF Inductors - SMD FIXED IND 7.3NH 0.45A 260 MOHM SMD
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TDK 863
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AUD 0.1116
Multiples of: 1

Multilayer Ceramic Inductor0402 (1005 METRIC)Shielded7.3 nH5 %450 mA260 mOhms - 55 C+ 125 C205.4 GHzStandard1 mm0.5 mm0.7 mm Ceramic MHQReel , Cut Tape
NLV25T-R47J-EF


RF Inductors - SMD 470nH 680mohms 350mA Wound Ferrite
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TDK 863
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AUD 0.1396
Multiples of: 1

Wirewound2.5 mm x 2 mm x 1.8 mmUnshielded470 nH5 %350 mA680 mOhms-- 40 C+ 105 C30350 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - EFReel , Cut Tape
PM1008-R33K-RC


Inductor RF Wirewound 0.33uH 10% 25MHz 45Q-Factor Ceramic 0.5A 1.05Ohm DCR 1008 T/R
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Bourns 863
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AUD 0.1804
Multiples of: 2000

Wirewound1008 (2520 METRIC)Unshielded330 nH10 %450 mA1.05 Ohms-- 55 C+ 125 C45570 MHzStandard2.5 mm2 mm1.6 mm-Ceramic PM1008Reel , Cut Tape
WCLA1005V1-121-R


RF Inductors - SMD WCLA Auto Chip IND 1005 120nH 2 Pads
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Eaton 863
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AUD 0.2189
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded120 nH5 %30 mA2.2 Ohms-- 40 C+ 125 C251.1 GHzStandard1.19 mm0.66 mm0.6 mm- AEC - Q200WCLAReel , Cut Tape
S1210R-101J


RF Inductors - SMD .1uH 5% .15ohm Shielded SMT Induc
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API Delevan 859
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AUD 3.0693
Multiples of: 1

Wirewound1210 (3225 METRIC)Shielded100 nH5 %1.13 A150 mOhms-- 55 C+ 125 C40375 MHzStandard3.51 mm2.66 mm2.57 mm-Iron S1210/RReel , Cut Tape
WCLA1608V1-680-R


RF Inductors - SMD WCLA Auto Chip IND 1608 68nH 2 Pads
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Eaton 858
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AUD 0.1913
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded68 nH5 %600 mA340 mOhms-- 40 C+ 125 C361.7 GHzStandard1.78 mm1.1 mm0.95 mm- AEC - Q200WCLAReel , Cut Tape
AL12A08N0KTR


RF Inductors - SMD 8nH 10% AIR CORE
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Kyocera AVX 855
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AUD 0.2706
Multiples of: 1

Wirewound3.05 mm x 3.18 mm x 3.68 mmUnshielded8 nH10 %4 A2.6 mOhms-- 40 C+ 125 C1405 GHzStandard3.68 mm3.05 mm3.18 mm-Air ALReel , Cut Tape
1210F-100J-01


RF Inductors - SMD Chip Inductor (Wire wound -open); 10H; Tol: 5%
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Fastron 851
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AUD 0.4327
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded10 uH5 % 4.3 Ohms     Standard3.8 mm3 mm2.4 mm FerriteAEC - Q2001210FReel , Cut Tape
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