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
  
                         
IMC1812ER270J


RF Inductors - SMD 27uh 5%
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Vishay 0
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AUD 1.0376

Multiples of: 1

Molded1812 (4532 METRIC) 27 uH  280 mOhms     Standard      IMCReel , Cut Tape
PM105-470K-RC


Inductor Power Bobbin Core 47uH 10% 1KHz 20Q-Factor Ferrite 1.25A 170mOhm DCR T/R
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Bourns 0
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AUD 1.0046

Multiples of: 1

Smd Power Inductor Unshielded47 uH10 %1.25 A180 mOhms - 30 C+ 100 C 10 MHz    9.8 mm  Pm105Reel
0402CS-8N7XJRW


RF Inductors - SMD 1005 8.7nH Unshld 5% 480mA 200mOhms AECQ2
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Coilcraft 0
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AUD 1.0067

Multiples of: 1

   8.7 nH                 
0402CS-82NXJRW


RF Inductors - SMD 1005 82nH Unshld 5% 50mA 1.55 Ohms AECQ2
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Coilcraft 0
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AUD 1.0067

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   82 nH                 
0603DC-R11XJRW


RF Inductors - SMD 0603 110nH 270mA 5% DCR=.725OhmsAEC-Q200
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Coilcraft 0
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AUD 1.0106

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Wirewound0603 (1608 METRIC)Unshielded110 nH5 %620 mA725 mOhms-- 40 C+ 125 C-1.25 GHzStandard1.7 mm0.99 mm0.89 mm-CeramicAEC - Q2000603DCReel , Cut Tape
0603DC-10NXJRW


RF Inductors - SMD 0603 10nH 1160mA 5% DCR=.06Ohms AEC-Q200
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Coilcraft 0
6 to 16 Weeks Calender.png

AUD 1.0106

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded10 nH5 %2.26 A60 mOhms-- 40 C+ 125 C-4.1 GHzStandard1.7 mm0.99 mm0.89 mm-CeramicAEC - Q2000603DCReel , Cut Tape
0603DC-3N9XJRW


RF Inductors - SMD 0603 3.9nH 1390mA 5% DCR=.04Ohms AEC-Q200
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Coilcraft 0
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AUD 1.0106

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded3.9 nH5 %2.8 A40 mOhms-- 40 C+ 125 C-11.25 GHzStandard1.7 mm0.99 mm0.89 mm-CeramicAEC - Q2000603DCReel , Cut Tape
0603DC-36NXJRW


RF Inductors - SMD 0603 36nH 740mA 5% DCR=.134OhmsAEC-Q200
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Coilcraft 0
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AUD 1.0119

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded36 nH5 %1.49 A134 mOhms-- 40 C+ 125 C-2.35 GHzStandard1.7 mm0.99 mm0.89 mm-CeramicAEC - Q2000603DCReel , Cut Tape
0603DC-9N1XJRW


RF Inductors - SMD 0603 9.1nH 1160mA 5% DCR=.06Ohms AEC-Q200
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Coilcraft 0
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AUD 1.0119

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded9.1 nH5 %2.26 A60 mOhms-- 40 C+ 125 C-4.5 GHzStandard1.7 mm0.99 mm0.89 mm-CeramicAEC - Q2000603DCReel , Cut Tape
0603DC-56NXJRW


RF Inductors - SMD 0603 56nH 490mA 5% DCR=.260OhmsAEC-Q200
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Coilcraft 0
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AUD 1.0119

Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded56 nH5 %1.03 A260 mOhms-- 40 C+ 125 C-1.85 GHzStandard1.7 mm0.99 mm0.89 mm-CeramicAEC - Q2000603DCReel , Cut Tape
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