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
  
                         
NLV32T-R39J-EFD


RF Inductors - SMD 390nH 450mohms 450mA Wound Fer AEC-Q200
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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.

TDK 1936
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AUD 0.17
Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded390 nH5 %450 mA450 mOhms-- 40 C+ 105 C30250 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
AISC-1206-12NJ-T


RF Inductors - SMD FIXED IND 12NH 1A 90 MOHM SMD
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ABRACON 1936
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AUD 0.4785
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Ceramic Wirewound RF Inductor1206 (3216 METRIC)Unshielded12 nH5 %1 A90 mOhms - 40 C+ 125 C403.2 GHzStandard3.56 mm2.16 mm1.52 mm Ceramic AISC - 1206Reel , Cut Tape
LQH44PN3R3MPRL


RF Inductors - SMD 3.3uH 2300mA 20%
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Murata 1935
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AUD 0.3021
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Wirewound4 mm x 4 mm x 1.65 mmUnshielded3.3 uH20 %2.3 A55 mOhms - 40 C+ 125 C 40 MHzStandard4 mm4 mm1.65 mm   LQH44PN_PRReel , Cut Tape
MLF2012C270M


RF Inductors - SMD 27uH
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TDK 1934
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AUD 0.078
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Multilayer0805 (2012 METRIC)Shielded27 uH20 %5 mA1 Ohms-- 55 C+ 125 C3033 MHzStandard2 mm1.25 mm1.25 mm-Ferrite MLFReel , Cut Tape
MLF2012E6R8KTD25


RF Inductors - SMD 6.8uH 650mohms 15mA +/-10% Fer AEC-Q200
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TDK 1933
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AUD 0.1026
Multiples of: 5

Multilayer0805 (2012 METRIC)Shielded6.8 uH10 %15 mA650 mOhms-- 55 C+ 125 C5060 MHzStandard2 mm1.25 mm1.25 mm-FerriteAEC - Q200MLFReel , Cut Tape
NLFV32T-101K-EFT


RF Inductors - SMD 100uH 2.2ohms 55mA +/-10%
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TDK 1933
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AUD 0.2155
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Wirewound1210 (3225 METRIC)Shielded100 uH10 %55 mA2.2 Ohms-- 40 C+ 105 C--Standard3.2 mm2.5 mm2.2 mm-Ferrite NLFV - EFTReel , Cut Tape
LQW2UAS39NG00L


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 1932
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AUD 0.1742
Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded39 nH2 %1 A150 mOhms-- 55 C+ 125 C601.5 GHzStandard2.62 mm2.45 mm1.83 mm-  LQWReel , Cut Tape
B82422H1682K


RF Inductors - SMD 6.8 UH 10%
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TDK 1932
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AUD 0.3538
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded6.8 uH10 %580 mA350 mOhms770 mA- 55 C+ 150 C835 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200B82422Reel , Cut Tape
AS0827N3JTR


RF Inductors - SMD 27.3nH 5% Square Air Core
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Kyocera AVX 1932
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AUD 0.3675
Multiples of: 1

Wirewound2.134 mm x 1.829 mm x 2.972 mmUnshielded27.3 nH5 %4.4 A10 mOhms-- 40 C+ 125 C1303.2 GHzStandard2.972 mm2.134 mm1.829 mm-Air ASReel , Cut Tape
LQW18ASR20J0ZD


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 1930
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AUD 0.1352
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded200 nH5 %200 mA1.98 Ohms-- 40 C+ 125 C25900 MHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
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