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
  
                         
MLF2012A2R2KTD25


RF Inductors - SMD 2.2uH 500mohms 50mA +/-10% Fer AEC-Q200
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TDK 3880
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AUD 0.1395
Multiples of: 1

Multilayer0805 (2012 METRIC)Shielded2.2 uH10 %50 mA500 mOhms-- 55 C+ 125 C45120 MHzStandard2 mm1.25 mm0.85 mm-FerriteAEC - Q200MLFReel , Cut Tape
AISC-Q0402-4N7J-T


RF Inductors - SMD IND 4.7nH 0.64A 130m?
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Abracon 3880
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AUD 0.1429
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded4.7 nH5 %640 mA130 mOhms - 40 C+ 125 C184.7 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
AISC-Q0402-3N9J-T


RF Inductors - SMD IND 3.9nH 0.84A 66m?
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Abracon 3880
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AUD 0.1429
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded3.9 nH5 %840 mA66 mOhms - 40 C+ 125 C195.8 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
AISC-Q0402-2N7J-T


RF Inductors - SMD IND 2.7nH 0.64A 120m?
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Abracon 3880
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AUD 0.1429
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded2.7 nH5 %640 mA120 mOhms - 40 C+ 125 C1610.4 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
AISC-Q0402-8N2J-T


RF Inductors - SMD IND 8.2nH 0.68A 104m?
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Abracon 3880
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AUD 0.1429
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded8.2 nH5 %680 mA104 mOhms - 40 C+ 125 C224.4 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
LQW18ANR36J8ZD


RF Inductors - SMD
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 3880
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AUD 0.144
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Wirewound0603 (1608 METRIC)Unshielded360 nH5 %190 mA3.98 Ohms-- 55 C+ 125 C251.05 GHzStandard1.65 mm0.99 mm0.9 mm- AEC - Q200LQWReel , Cut Tape
MLJ1608WR47KT000


RF Inductors - SMD 470nH 0.38ohms 600mA 10% 190MHz
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TDK 3880
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AUD 0.1449
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NFC Inductor0603 (1608 METRIC)Shielded470 nH10 %400 mA500 mOhms600 mA- 55 C+ 125 C15260 MHzStandard1.6 mm0.8 mm0.8 mm-Ferrite MLJReel , Cut Tape
MLF2012DR39KTD25


RF Inductors - SMD 390nH 450mohms 200mA +/-10% Fer AEC-Q200
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TDK 3880
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AUD 0.146
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Multilayer0805 (2012 METRIC)Shielded390 nH10 %200 mA450 mOhms-- 55 C+ 125 C25250 MHzStandard2 mm1.25 mm0.85 mm-FerriteAEC - Q200MLFReel , Cut Tape
NLV32T-151J-EFD


RF Inductors - SMD 150uH 15ohms 65mA Wound Fer AEC-Q200
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TDK 3880
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AUD 0.1467
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Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded150 uH5 %65 mA15 Ohms-- 40 C+ 105 C208 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
LQW18AN18NJ1ZD


RF Inductors - SMD
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This product is classified as Large/Heavy, additional shipping charges may apply. A customer service representative may contact you after ordering to confirm exact shipping charges.

Murata 3880
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AUD 0.1474
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Wirewound0603 (1608 METRIC)Unshielded18 nH5 %700 mA85 mOhms-- 55 C+ 125 C423.5 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
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