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-R56J-EFD


RF Inductors - SMD 560nH 550mohms 450mA Wound Fer AEC-Q200
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TDK 44620
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AUD 0.1517
Multiples of: 2000

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded560 nH5 %450 mA550 mOhms-- 40 C+ 105 C30180 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
CIGT252010LMR47MNE


RF Inductors - SMD CIGT,Thin Film,1008,0.47uH,1.0?,7 embossed,-20 20%
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SAMSUNG 44310
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AUD 0.132
Multiples of: 1

Thin Film  470 nH20 %              CIGTReel , Cut Tape
LQP03HQ13NJ02D


RF Inductors - SMD
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Murata 43754
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AUD 0.0792
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded13 nH5 %300 mA500 mOhms-- 55 C+ 125 C204 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
BSCQ000603031N0B00


RF Inductors - SMD 1nH RDC=.07Ohms 850mA
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Pulse 43650
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AUD 0.0154
Multiples of: 15000

 0.6 mm x 0.3 mm x 0.3 mmShielded1 nH0.1 nH850 mA70 mOhms850 mA- 55 C+ 125 C1410 GHzStandard0.6 mm0.3 mm0.3 mm Ceramic BSCQReel , Cut Tape
ILSB1206ERR18K


RF Inductors - SMD .18uH 10%
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Vishay 43650
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AUD 0.1151
Multiples of: 1

Established Reliability1206 (3216 METRIC)Shielded180 nH10 %250 mA400 mOhms-- 55 C+ 125 C20213 MHzStandard3.2 mm1.6 mm1.1 mm-  ILSB - 1206Reel , Cut Tape
LQP03HQR12H02D


RF Inductors - SMD
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Murata 43630
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AUD 0.104
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded120 nH3 %80 mA8 Ohms-- 55 C+ 125 C10800 MHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
LCCI0201S1N6GTAR


RF Inductors - SMD 1.6nH Tol 0.3nH 0201 500mA DCR=.18 Ohms
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Kyocera AVX 43439
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AUD 0.0101
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded1.6 nH0.3 nH500 mA180 mOhms-- 40 C+ 85 C410 GHzStandard0.6 mm0.3 mm0.3 mm-  LCCIReel , Cut Tape
LCCI0201B0N3GTAR


RF Inductors - SMD .3nH Tol 0.1nH 0201 850mA DCR=.07 Ohms
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Kyocera AVX 43258
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AUD 0.0105
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded300 pH0.1 nH850 mA70 mOhms-- 40 C+ 85 C410 GHzStandard0.6 mm0.3 mm0.3 mm-  LCCIReel , Cut Tape
LQP03HQ4N7J02D


RF Inductors - SMD 4.7 NH 5%
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Murata 29955
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AUD 0.0676
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded4.7 nH5 %400 mA250 mOhms-- 55 C+ 125 C207 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
LQG15HS1N2S02D


RF Inductors - SMD 1.2 NH +-.3NH
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Murata 2231
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AUD 0.0094
Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded1.2 nH0.3 nH1 A70 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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