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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Enter Qty TypePackage / CaseShieldingInductanceToleranceMaximum DC CurrentMaximum DC ResistanceSaturation CurrentMinimum Operating TemperatureMaximum Operating TemperatureQ MinimumSelf Resonant FrequencyTerminationLengthWidthHeightDiameterCore MaterialQualificationSeriesPackaging
  
                         
0603LS-181XJRC


RF Inductors - SMD 0603 180nH Unshld 5% 150mOhms AEC-Q200
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AUD 1.3713

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                  AEC - Q2000603LSReel , Cut Tape
0402HPH-56NXGRW


RF Inductors - SMD
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AUD 1.3713

Multiples of: 1

                     
0402DC-43NXGRW


RF Inductors - SMD 1005 43nH Unshld 2% 640mA 430mOhms
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AUD 1.3913

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Wirewound0402 (1005 METRIC)Unshielded43 nH2 %640 mA430 mOhms-- 40 C+ 125 C543.82 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
0603AF-102XJRW


RF Inductors - SMD 1608 1000nH Unshld 5% 400mA 840mOhms
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AUD 1.4044

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded1 uH5 %400 mA840 mOhms-- 40 C+ 85 C17400 MHzStandard1.8 mm1.12 mm0.91 mm-Ferrite 0603AFReel , Cut Tape
0603HL-511XJRC


RF Inductors - SMD 0603 510nH Unshld 5% 300mA 1.2Ohms
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AUD 1.4044

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 0603 (1608 METRIC)Unshielded510 nH5 %300 mA1.2 Ohms - 40 C+ 125 C12340 MHzStandard1.8 mm1.19 mm0.94 mm Ceramic 0603HLReel , Cut Tape
0603HL-561XJRC


RF Inductors - SMD 0603 560nH Unshld 5% 300mA 1.35Ohms
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Coilcraft 0
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AUD 1.4044

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded560 nH5 %300 mA1.35 Ohms-- 40 C+ 125 C12330 MHzStandard1.8 mm1.19 mm0.94 mm-Ceramic 0603HLReel , Cut Tape
0603HL-821XJRC


RF Inductors - SMD 0603 820nH Unshld 5% 190mA 2.45Ohms
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AUD 1.4044

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Wirewound0603 (1608 METRIC)Unshielded820 nH5 %190 mA2.45 Ohms-- 40 C+ 125 C14290 MHzStandard1.8 mm1.19 mm0.94 mm-Ceramic 0603HLReel , Cut Tape
0603HL-332XJRC


RF Inductors - SMD 0603 3300nH Unshld 5% 110mA 9.1Ohms
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AUD 1.4044

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Wirewound0603 (1608 METRIC)Unshielded3.3 uH5 %110 mA9.1 Ohms-- 40 C+ 125 C18135 MHzStandard1.8 mm1.19 mm0.94 mm-Ceramic 0603HLReel , Cut Tape
0603AF-472XJRW


RF Inductors - SMD 1608 4700nH Unshld 5% 260mA 1.5 Ohms
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AUD 1.4044

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Wirewound0603 (1608 METRIC)Unshielded4.7 uH5 %260 mA1.5 Ohms-- 40 C+ 85 C1660 MHzStandard1.8 mm1.12 mm0.91 mm-Ferrite 0603AFReel , Cut Tape
1812SMS-82NJLC


RF Inductors - SMD 1812 82nH Unshld 5% 2.5A 9.4mOhms AECQ2
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AUD 1.408

Multiples of: 1

Wirewound1812 (4532 METRIC)Unshielded82 nH5 %2.5 A9.4 mOhms-- 40 C+ 125 C1001.3 GHzStandard6.35 mm4.95 mm4.2 mm-AirAEC - Q2001812SMSReel , Cut Tape
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