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
  
                         
LQW15AN33NG00D


RF Inductors - SMD 33 NH 2%
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Murata 159526
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AUD 0.0595
Multiples of: 20

Wirewound0402 (1005 METRIC)Unshielded33 nH2 %260 mA630 mOhms-- 55 C+ 125 C253.2 GHzStandard1 mm0.5 mm0.5 mm-  LQWReel , Cut Tape
MHQ0603P0N8CT000


RF Inductors - SMD IND 0201 0.8nH S-HQ SMD RF IND
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TDK 150922
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AUD 0.0448
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded800 pH0.2 nH1 A70 mOhms-- 55 C+ 125 C-20 GHzStandard0.65 mm0.35 mm0.35 mm Ceramic MHQ - PReel , Cut Tape
MLG0603P1N0BTD25


RF Inductors - SMD IND 0201 1.0nH Hi-Q AEC Q200 RF IND
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TDK 145500
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AUD 0.0155
Multiples of: 15000

Multilayer0201 (0603 METRIC)Unshielded1 nH0.1 nH1 A70 mOhms-- 55 C+ 125 C1420 GHzStandard0.6 mm0.3 mm0.3 mm-CeramicAEC - Q200MLG - PReel , Cut Tape
LQP03TQ5N6H02D


RF Inductors - SMD 5.6nH 350mA 0201 (0603 metric) SUGGESTED ALT LQP03HQ5N6H02D
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Murata 145307
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AUD 0.0276
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded5.6 nH3 %350 mA390 mOhms - 55 C+ 125 C176 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
BSCH0010050510NJCS


RF Inductors - SMD 1005 10nH
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Pulse 134497
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AUD 0.0155
Multiples of: 1

 1 mm x 0.5 mm x 0.5 mmShielded10 nH5 % 260 mOhms300 mA- 55 C+ 125 C83.9 GHzStandard1 mm0.5 mm0.5 mm-Ceramic BSCHReel , Cut Tape
LQG15HS4N7S02D


RF Inductors - SMD 4.7 NH 3%
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Murata 132890
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AUD 0.0114
Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded4.7 nH0.3 nH700 mA160 mOhms - 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
CIGT201610LHR24MNE


RF Inductors - SMD CIGT,Thin Film,0806,0.24uH,1.0?,7 embossed,-20 20%
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SAMSUNG 132581
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AUD 0.1138
Multiples of: 1

Thin Film  240 nH20 %              CIGTReel , Cut Tape
LQP03TN15NH02D


RF Inductors - SMD 15 NH 3%
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Murata 130659
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AUD 0.0083
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded15 nH3 %250 mA700 mOhms - 55 C+ 125 C122.6 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQW15AN2N6G8ZD


RF Inductors - SMD
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Murata 126950
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AUD 0.1323
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded2.6 nH2 %1.95 A35 mOhms-- 55 C+ 125 C3014.5 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
BSCH000603038N2J00


RF Inductors - SMD 0603 8.2nH
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Pulse 123990
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AUD 0.0164
Multiples of: 1

 0.6 mm x 0.3 mm x 0.3 mmShielded8.2 nH5 % 450 mOhms230 mA- 55 C+ 125 C43.4 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic BSCHReel , Cut Tape
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