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
  
                         
LQP03TN47NH02D


RF Inductors - SMD 47 NH 3%
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Murata 30114
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AUD 0.0242
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Thin Film0201 (0603 METRIC)Unshielded47 nH3 %100 mA3.6 Ohms - 55 C+ 125 C91.3 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
Hot ATFC-0402-3N3-BT


RF Inductors - SMD
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ABRACON 29909
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AUD 0.0163
Multiples of: 1

Thin Film Chip Inductor0402 (1005 METRIC)Unshielded3.3 nH0.1 nH380 mA450 mOhms - 45 C+ 85 C136 GHzStandard1 mm0.5 mm0.32 mm Ceramic ATFC - 0402Reel , Cut Tape
AIML-0603-4R7K-T


RF Inductors - SMD 4.7 UH +/-10%
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ABRACON 29876
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AUD 0.0409
Multiples of: 4000

Multilayer0603 (1608 METRIC)Shielded4.7 uH10 %15 mA2.1 Ohms - 55 C+ 125 C3550 MHzStandard1.6 mm0.8 mm0.8 mm Ferrite AIML - 0603Reel , Cut Tape
NLV25T-100J-PF


RF Inductors - SMD SUGGESTED ALTERNATE NLV25T-100J-EF
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TDK 29857
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AUD 0.1224
Multiples of: 1

Wirewound Unshielded10 uH5 %155 mA3.5 Ohms-- 40 C+ 105 C2533 MHzStandard2.5 mm2 mm1.8 mm-Ferrite NLV25 - PFReel , Cut Tape
LQW15AN10NG80D


RF Inductors - SMD 10 NH 2%
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Murata 29662
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AUD 0.0628
Multiples of: 10

Wirewound0402 (1005 METRIC)Unshielded10 nH2 %1.4 A81 mOhms-- 55 C+ 125 C316 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQP03TN2N9B02D


RF Inductors - SMD 2.9 NH +-.1NH
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Murata 29585
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AUD 0.0038
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded2.9 nH0.1 nH500 mA200 mOhms - 55 C+ 125 C149.5 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
Hot MLF1005GR82JT000


RF Inductors - SMD 1mm x 0.5mm x 0.5mm, -55 to +125 degC, 40mA, 0.82?H, 590mohm
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TDK 29230
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AUD 0.1614
Multiples of: 1

Multilayer0402 (1005 METRIC)Shielded820 nH5 %40 mA590 mOhms-- 55 C+ 125 C30320 MHzStandard1 mm0.5 mm0.5 mm-Ferrite MLFReel , Cut Tape
LQW18AS24NG00D


RF Inductors - SMD
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Murata 29203
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AUD 0.0888
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded24 nH2 %700 mA135 mOhms-- 40 C+ 125 C362.65 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQP03TN2N8B02D


RF Inductors - SMD 2.8 NH
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Murata 29100
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AUD 0.004
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded2.8 nH0.1 nH500 mA200 mOhms-- 55 C+ 125 C149.5 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
AISC-0402-3N3J-T


RF Inductors - SMD FIXED IND 3.3NH 840MA 66 MOHM
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ABRACON 8717
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AUD 0.0317
Multiples of: 1

Smd Ceramic Wire - Wound Chip Inductors0402 (1005 METRIC)Unshielded3.3 nH5 %840 mA66 mOhms - 40 C+ 125 C207000 MHz     Ceramic Aisc - 0402Reel
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