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
  
                         
MLF1005G1R8JTD25


RF Inductors - SMD 0402 1.8uH 5% AEC-Q200
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TDK 15459
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AUD 0.1673
Multiples of: 1

Multilayer0402 (1005 METRIC)Shielded1.8 uH5 %30 mA1.05 Ohms-- 55 C+ 125 C30180 MHzStandard1 mm0.5 mm0.5 mm-FerriteAEC - Q200MLFReel , Cut Tape
B82422A3561K100


RF Inductors - SMD SMT-INDUCTOR 1210 0.56UH 10%, AECQ200
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TDK 5857
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AUD 0.3051
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded560 nH10 %150 mA2.2 Ohms-- 55 C+ 145 C22400 MHzStandard3.2 mm2.5 mm2 mm-CeramicAEC - Q200B82422AReel , Cut Tape
LQW18AN30NG8ZD


RF Inductors - SMD
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Murata 5853
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AUD 0.1777
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Wirewound0603 (1608 METRIC)Unshielded30 nH2 %1.1 A120 mOhms-- 55 C+ 125 C402.88 GHzStandard1.65 mm0.99 mm0.9 mm--AEC - Q200LQWReel , Cut Tape
LQP02HQ4N2B02E


RF Inductors - SMD
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Murata 5844
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AUD 0.1069
Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded4.2 nH0.1 nH350 mA350 mOhms-- 55 C+ 125 C146.9 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQW18AN33NJ80D


RF Inductors - SMD
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Murata 5842
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AUD 0.0966
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded33 nH5 %1.1 A110 mOhms-- 55 C+ 125 C403.15 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
KLZ2012MHR2R2HTD25


RF Inductors - SMD 2.2uH 2MHz 20% 2012 AEC-Q200
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TDK 5841
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AUD 0.1469
Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded2.2 uH20 %600 mA160 mOhms400 mA- 55 C+ 150 C--Flexible (Soft)2 mm1.25 mm1.25 mm-FerriteAEC - Q200KLZ - HRReel , Cut Tape
MLF1005G1R8JT000


RF Inductors - SMD 1mm x 0.5mm x 0.5mm, -55 to +125 degC, 30mA, 1.8?H, 1.05ohm
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TDK 5834
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AUD 0.1477
Multiples of: 1

Multilayer0402 (1005 METRIC)Shielded1.8 uH5 %30 mA1.05 Ohms-- 55 C+ 125 C30180 MHzStandard1 mm0.5 mm0.5 mm-Ferrite MLFReel , Cut Tape
MCQ1V3216-R470-R


RF Inductors - SMD Multi H Q,IND 470nH Q30 200mA 2PADS SMT
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Eaton 5832
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AUD 0.0551
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Multilayer1206 (3216 METRIC)Unshielded470 nH10 %200 mA500 mOhms-- 40 C+ 85 C30125 MHzStandard3.2 mm1.6 mm0.9 mm-  MCQ1VReel , Cut Tape
NLV32T-150J-EF


RF Inductors - SMD 15uH 2.8ohms 130mA Wound Ferrite
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TDK 3821
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AUD 0.0457
Multiples of: 10

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded15 uH5 %130 mA2.8 Ohms-- 40 C+ 105 C3020 MHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
LQW18CNR56J00D


RF Inductors - SMD 560 NH 5%
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Murata 1906
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AUD 0.1329
Multiples of: 5

Wirewound0603 (1608 METRIC)Unshielded560 nH5 %450 mA480 mOhms-- 40 C+ 85 C-540 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite LQWReel , Cut Tape
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