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
  
                         
LQW15AN56NJ00D


RF Inductors - SMD 56 NH 5%
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Murata 22368
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AUD 0.0356
Multiples of: 20

Wirewound0402 (1005 METRIC)Unshielded56 nH5 %200 mA1.17 Ohms-- 55 C+ 125 C252.8 GHzStandard1 mm0.5 mm0.5 mm-  LQWReel , Cut Tape
MLF1608DR47JTD25


RF Inductors - SMD 470nH 950mohms 100mA +/-5% Fer AEC-Q200
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TDK 3176
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AUD 0.0926
Multiples of: 5

Multilayer0603 (1608 METRIC)Shielded470 nH5 %100 mA950 mOhms-- 55 C+ 125 C15260 MHzStandard1.6 mm0.8 mm0.8 mm-FerriteAEC - Q200MLFReel , Cut Tape
AIMC-0402-12NJ-T


RF Inductors - SMD FIXED IND 12NH 300MA 500 MOHM
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ABRACON 3168
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AUD 0.0256
Multiples of: 1

Multilayer Ceramic Chip Inductor0402 (1005 METRIC)Shielded12 nH5 %300 mA500 mOhms - 55 C+ 125 C92.8 GHzStandard1 mm0.5 mm0.5 mm Ceramic AIMC - 0402Reel , Cut Tape
MLF2012A2R2KT000


Inductor RF Chip Shielded Multi-Layer 2.2uH 10% 10MHz 45Q-Factor Ferrite 50mA 500mOhm DCR 0805 T/R
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TDK 3162
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AUD 0.0423
Multiples of: 20

Multilayer0805 (2012 METRIC)Shielded2.2 uH10 %50 mA500 mOhms-- 55 C+ 125 C45120 MHzStandard2 mm1.25 mm0.85 mm-Ferrite MLFReel , Cut Tape
MHQ0603P24NHTD25


RF Inductors - SMD 0201 24nH Tol 3% AEC-Q200
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TDK 3162
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AUD 0.0789
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded24 nH3 %160 mA2.2 Ohms-- 55 C+ 125 C163.1 GHzStandard0.65 mm0.35 mm0.35 mm-CeramicAEC - Q200MHQ - PReel , Cut Tape
LQW18ANR11G0ZD


RF Inductors - SMD
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Murata 3155
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AUD 0.126
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded110 nH2 %200 mA1.2 Ohms-- 55 C+ 125 C321.7 GHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
BWCM0012070711NG00


RF Inductors - SMD 0402 11nH
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Pulse 3152
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AUD 0.1273
Multiples of: 1

 1.6 mm x 0.7 mm x 0.66 mmUnshielded11 nH2 %500 mA140 mOhms500 mA- 55 C+ 125 C305.5 GHzStandard1.2 mm0.7 mm0.66 mm-Ceramic BWCMReel , Cut Tape
B82496C3339A


RF Inductors - SMD 3.3nH 1200mA 0.3nH 1.6x0.8mm SMD
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TDK 3150
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AUD 0.2083
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded3.3 nH0.3 nH1.2 A60 mOhms-- 55 C+ 150 C149 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200SIMID - CReel , Cut Tape
LQW18ANR47J0ZD


RF Inductors - SMD
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Murata 3143
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AUD 0.1192
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded470 nH5 %75 mA7 Ohms-- 55 C+ 125 C30700 MHzStandard1.6 mm0.8 mm0.8 mm- AEC - Q200LQWReel , Cut Tape
NLV32T-047J-EF


RF Inductors - SMD 47nH 300mohms 450mA Wound Ferrite
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TDK 3133
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AUD 0.0522
Multiples of: 10

Wirewound3.2 mm x 2.5 mm x 2.2 mmUnshielded47 nH5 %450 mA300 mOhms-- 40 C+ 105 C261.2 GHzStandard3.2 mm2.5 mm2.2 mm-Ferrite NLV32 - EFReel , Cut Tape
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