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
  
                         
1210R-470K


RF Inductors - SMD 0.047uH 10%
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API Delevan 919
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AUD 2.1548
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded47 nH10 %636 mA300 mOhms-- 55 C+ 125 C30800 MHzStandard3.51 mm2.67 mm2.57 mm-  1210/RReel , Cut Tape
MHQ1005075HA13NHTD25


RF Inductors - SMD FIXED IND 13NH 0.3A 500 MOHM SMD
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TDK 916
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AUD 0.11
Multiples of: 1

Multilayer Ceramic Inductor0402 (1005 METRIC)Shielded13 nH3 %300 mA500 mOhms - 55 C+ 125 C203.8 GHzStandard1 mm0.5 mm0.7 mm Ceramic MHQReel , Cut Tape
MHQ1005075HA1N6STD25


RF Inductors - SMD FIXED IND 1.6NH 1A 30 MOHM SMD
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TDK 916
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AUD 0.11
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Multilayer Ceramic Inductor0402 (1005 METRIC)Shielded1.6 nH0.3 nH1 A30 mOhms - 55 C+ 125 C2020 GHzStandard1 mm0.5 mm0.7 mm Ceramic MHQReel , Cut Tape
MHQ1005075HA47NJTD25


RF Inductors - SMD FIXED IND 47NH 0.18A 1.3 OHM SMD
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TDK 916
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AUD 0.1116
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Multilayer Ceramic Inductor0402 (1005 METRIC)Shielded47 nH5 %180 mA1.3 Ohms - 55 C+ 125 C201.6 GHzStandard1 mm0.5 mm0.7 mm Ceramic MHQReel , Cut Tape
S1008R-103J


RF Inductors - SMD 10uH 5% 2.1ohm Shielded SMT Induc
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API Delevan 916
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AUD 5.5392
Multiples of: 1

Wirewound1008 (2520 METRIC)Shielded10 uH5 %230 mA2.1 Ohms-- 55 C+ 125 C3029 MHzStandard2.92 mm2.66 mm2.41 mm-Ferrite S1008/RReel , Cut Tape
AIAC-4125C-R090J-T


RF Inductors - SMD FIXED IND 90NH 3.5A 14 MOHM SMD
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ABRACON 915
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AUD 1.3342
Multiples of: 1

SMT Air Coil Inductor9 mm x 4.4 mm x 4.6 mmUnshielded90 nH5 %3.5 A14 mOhms - 40 C+ 125 C1001 GHzStandard9 mm4.4 mm4.6 mm Air AIAC - 4125CReel , Cut Tape
LQW18AN56NG8ZD


RF Inductors - SMD
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Murata 911
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AUD 0.1306
Multiples of: 5

Wirewound0603 (1608 METRIC)Unshielded56 nH2 %770 mA260 mOhms-- 55 C+ 125 C382.6 GHzStandard1.65 mm0.99 mm0.9 mm--AEC - Q200LQWReel , Cut Tape
AISC-1210-68NJ-T


RF Inductors - SMD FIXED IND 68NH 900MA 150 MOHM
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ABRACON 910
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AUD 0.5344
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Wirewound1210 (3225 METRIC)Unshielded68 nH5 %900 mA150 mOhms - 40 C+ 125 C551.2 GHzStandard3.65 mm2.95 mm2.7 mm Ceramic AISC - 1210Reel , Cut Tape
NLV32T-R12J-EFD


RF Inductors - SMD 120nH 220mohms 450mA Wound Fer AEC-Q200
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TDK 907
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AUD 0.1673
Multiples of: 1

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded120 nH5 %450 mA220 mOhms-- 40 C+ 105 C30500 MHzStandard3.2 mm2.5 mm2.2 mm-FerriteAEC - Q200NLV32 - EFDReel , Cut Tape
LQW18AN24NJ00D


RF Inductors - SMD 24 NH 5%
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Murata 873
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AUD 0.0396
Multiples of: 20

Wirewound0603 (1608 METRIC)Unshielded24 nH5 %500 mA210 mOhms-- 55 C+ 125 C403.8 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
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