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
  
                         
0402HP-22NXJRW


RF Inductors - SMD 1005 22nH Unshld 5% 800mA 160mOhms
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Coilcraft 0
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AUD 1.2259
Multiples of: 1

   22 nH                 
PM105-181K-RC


RF Inductors - SMD 180uH 10%
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Bourns 0
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AUD 1.2283
Multiples of: 1

Smd Power Inductor Unshielded180 uH10 %720 mA630 mOhms    5 MHz    9.8 mm  Pm105Cut Tape
0402DC-2N4XJRW


RF Inductors - SMD 1005 2.4nH Unshld 5% 850mA 170mOhms
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Coilcraft 0
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AUD 1.2299
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded2.4 nH5 %850 mA170 mOhms-- 40 C+ 125 C8016.1 GHzStandard1.11 mm0.66 mm0.65 mm-CeramicAEC - Q200DCReel , Cut Tape
1008LS-182XJLC


RF Inductors - SMD 1008 1.8uH Unshld 5% 600mA 840mOhms AECQ
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AUD 1.2377
Multiples of: 1

Wirewound1008 (2520 METRIC)Unshielded1.8 uH5 %600 mA840 mOhms-- 40 C+ 85 C37170 MHzStandard2.92 mm2.79 mm2.03 mm-CeramicAEC - Q2001008LSReel , Cut Tape
0906-3JLC


RF Inductors - SMD 2.55nH Unshld 5% 1.6A 5mOhms
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Coilcraft 0
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AUD 1.24
Multiples of: 1

Wirewound3.43 mm x 1.52 mm x 2.41 mmUnshielded2.55 nH5 %1.6 A5 mOhms-- 40 C+ 125 C1008.2 GHzStandard2.41 mm3.43 mm1.52 mm-Air 0906Reel , Cut Tape
1606-10JLC


RF Inductors - SMD 12.55nH Unshld 5% 1.6A 14mOhms
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Coilcraft 0
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AUD 1.2499
Multiples of: 1

Wirewound3.43 mm x 1.58 mm x 4.19 mmUnshielded12.55 nH5 %1.6 A14 mOhms-- 40 C+ 125 C1004.6 GHzStandard4.19 mm3.43 mm1.58 mm-Air 1606Reel , Cut Tape
1606-7JLC


RF Inductors - SMD 7.15nH Unshld 5% 1.6A 10mOhms
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Coilcraft 0
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AUD 1.2646
Multiples of: 1

Wirewound3.43 mm x 1.58 mm x 4.19 mmUnshielded7.15 nH5 %1.6 A10 mOhms-- 40 C+ 125 C1006 GHzStandard4.19 mm3.43 mm1.58 mm-Air 1606Reel , Cut Tape
1606-9JLC


RF Inductors - SMD 9.85nH Unshld 5% 1.6A 13mOhms
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Coilcraft 0
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AUD 1.2646
Multiples of: 1

Wirewound3.43 mm x 1.58 mm x 4.19 mmUnshielded9.85 nH5 %1.6 A13 mOhms-- 40 C+ 125 C1005.2 GHzStandard4.19 mm3.43 mm1.58 mm-Air 1606Reel , Cut Tape
1606-6JLC


RF Inductors - SMD 5.6nH Unshld 5% 1.6A 9mOhms
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Coilcraft 0
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AUD 1.2646
Multiples of: 1

Wirewound3.43 mm x 1.58 mm x 4.19 mmUnshielded5.6 nH5 %1.6 A9 mOhms-- 40 C+ 125 C1006.5 GHzStandard4.19 mm3.43 mm1.58 mm-Air 1606Reel , Cut Tape
0906-5JLC


RF Inductors - SMD 5.4nH Unshld 5% 1.6A 8mOhms
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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.

Coilcraft 0
6 to 16 Weeks Calender.png

AUD 1.2646
Multiples of: 1

Wirewound3.43 mm x 1.52 mm x 2.41 mmUnshielded5.4 nH5 %1.6 A8 mOhms-- 40 C+ 125 C1007 GHzStandard2.41 mm3.43 mm1.52 mm-Air 0906Reel , Cut Tape
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