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
  
                         
MLF2012A3R9KTD25


RF Inductors - SMD 3.9uH 650mohms 30mA +/-10% Fer AEC-Q200
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TDK 3861
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AUD 0.2205
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Multilayer0805 (2012 METRIC)Shielded3.9 uH10 %30 mA650 mOhms-- 55 C+ 125 C4580 MHzStandard2 mm1.25 mm1.25 mm-FerriteAEC - Q200MLFReel , Cut Tape
LQG15HS1N6B02D


RF Inductors - SMD 1.6 NH
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Murata 3860
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AUD 0.0353
Multiples of: 20

Multilayer0402 (1005 METRIC)Unshielded1.6 nH0.1 nH1 A70 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
AISC-Q0402-3N9J-T


RF Inductors - SMD IND 3.9nH 0.84A 66m?
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Abracon 3860
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AUD 0.1241
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Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded3.9 nH5 %840 mA66 mOhms - 40 C+ 125 C195.8 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
AISC-Q0402-22NG-T


RF Inductors - SMD IND 22nH 0.4A 300m?
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Abracon 3860
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AUD 0.1399
Multiples of: 1

Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded22 nH2 %400 mA300 mOhms - 40 C+ 125 C252.8 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
AISC-Q0402-11NG-T


RF Inductors - SMD IND 11nH 0.64A 120m?
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Abracon 3860
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AUD 0.143
Multiples of: 1

Ceramic Wirewound RF Inductor0402 (1208 METRIC)Unshielded11 nH2 %640 mA120 mOhms - 40 C+ 125 C243.68 GHzStandard1.27 mm0.76 mm0.61 mm   AISC - Q0402Reel , Cut Tape
WCLA1608V1-100-R


RF Inductors - SMD WCLA Auto Chip IND 1608 10nH 2 Pads
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Eaton 3860
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AUD 0.2052
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded10 nH5 %700 mA130 mOhms-- 40 C+ 125 C314.8 GHzStandard1.78 mm1.1 mm0.95 mm- AEC - Q200WCLAReel , Cut Tape
0603AQC-R25J-01


RF Inductors - SMD Wire-wound Ceramic Chip Inductor AEC-200
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Fastron 3860
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AUD 0.2231
Multiples of: 1

Chip Inductor0603 (1608 METRIC)Unshielded250 nH5 %300 mA1.65 Ohms - 40 C+ 140 C351 GHzStandard1.7 mm1.12 mm1.05 mm CeramicAEC - Q200 Reel , Cut Tape
ILSB0805ERR27K


RF Inductors - SMD .27uH 10%
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Vishay 3856
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AUD 0.1293
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Established Reliability0805 (2012 METRIC)Shielded270 nH10 %250 mA500 mOhms-- 55 C+ 125 C20173 MHzStandard2 mm1.25 mm0.9 mm-  ILSB - 0805Reel , Cut Tape
WCLA1608V1-560-R


RF Inductors - SMD WCLA Auto Chip IND 1608 56nH 2 Pads
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Eaton 3856
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AUD 0.2052
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Wirewound0603 (1608 METRIC)Unshielded56 nH5 %600 mA280 mOhms-- 40 C+ 125 C381.9 GHzStandard1.78 mm1.1 mm0.95 mm- AEC - Q200WCLAReel , Cut Tape
PE-0402CL560JTT


RF Inductors - SMD 0402 56nH 200mA DCR=12000mOhms RF
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Pulse 3855
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AUD 0.0276
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded56 nH5 %200 mA1.2 Ohms-- 55 C+ 125 C8750 MHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
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