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
  
                         
LQP03HQ1N2B02D


RF Inductors - SMD 1.2 NH
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Murata 27034
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AUD 0.0879
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Thin Film0201 (0603 METRIC)Unshielded1.2 nH0.1 nH1.1 A40 mOhms - 55 C+ 125 C2013 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
MLF1608E120MTD00


RF Inductors - SMD 1.6mm x 0.8mm x 0.8mm, -55 to +125 degC, 10mA, 12?H, 1.8ohm
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TDK 2346
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AUD 0.0755
Multiples of: 1

Multilayer Unshielded12 uH20 %10 mA1.8 Ohms-- 55 C+ 125 C-45 MHzStandard1.6 mm0.8 mm0.95 mm-Ferrite MLFReel , Cut Tape
AISC-0603-R0062J-T


RF Inductors - SMD FIXED IND 6.2NH 700MA 95 MOHM
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ABRACON 2337
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AUD 0.0292
Multiples of: 5

Wirewound0603 (1812 METRIC)Unshielded6.2 nH5 %700 mA95 mOhms - 40 C+ 125 C296 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - 0603Reel , Cut Tape
MCQ1V3216-R390-R


RF Inductors - SMD Multi H Q,IND 390nH Q30 200mA 2PADS SMT
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Eaton 2332
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AUD 0.0427
Multiples of: 1

 1206 (3216 METRIC)Shielded390 nH10 %200 mA500 mOhms - 40 C+ 85 C30135 MHzStandard3.2 mm1.6 mm0.9 mm   MCQ1VReel , Cut Tape
ILSB0603ER6R8K


RF Inductors - SMD 6.8uH 10%
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Vishay 2327
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AUD 0.1232
Multiples of: 1

Established Reliability0603 (1608 METRIC)Shielded6.8 uH10 %15 mA1.7 Ohms-- 55 C+ 125 C3020 MHzStandard1.6 mm0.8 mm0.8 mm-  ILSB - 0603Reel , Cut Tape
MLF1608E6R8KTD25


RF Inductors - SMD 6.8uH 1.3ohms 15mA +/-10% Fer AEC-Q200
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TDK 2322
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AUD 0.1224
Multiples of: 1

Multilayer0603 (1608 METRIC)Shielded6.8 uH10 %15 mA1.3 Ohms-- 55 C+ 125 C3560 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
NLV32T-180J-EFD


RF Inductors - SMD 18uH 3.3ohms 120mA Wound Fer AEC-Q200
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TDK 2306
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AUD 0.1517
Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded18 uH5 %120 mA3.3 Ohms-- 40 C+ 105 C3020 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
0805AS-056J-01


RF Inductors - SMD 56nH 200 MHz 5% Tol
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Fastron 2292
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AUD 0.2017
Multiples of: 1

Wirewound0805 (2012 METRIC)Unshielded56 nH5 %500 mA340 mOhms-- 40 C+ 150 C641.55 GHzStandard2.3 mm1.8 mm1.6 mm-CeramicAEC - Q2000805ASReel , Cut Tape
MLF2012A3R3M


RF Inductors - SMD 3.3uH
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TDK 2289
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AUD 0.0908
Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded3.3 uH20 %50 mA600 mOhms-- 55 C+ 125 C4590 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
AISC-0603-R022J-T


RF Inductors - SMD FIXED IND 22NH 490MA 190 MOHM
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ABRACON 816
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AUD 0.1413
Multiples of: 1

Wirewound0603 (1812 METRIC)Unshielded22 nH5 %490 mA190 mOhms - 40 C+ 125 C384.6 GHzStandard1.8 mm1.12 mm1.02 mm Ceramic AISC - 0603Reel , Cut Tape
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