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
  
                         
AIML-0603-1R0K-T


RF Inductors - SMD FIXED IND 1UH 25MA 600 MOHM SMD
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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.

ABRACON 72135
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AUD 0.0379
Multiples of: 1

Multilayer0603 (1608 METRIC)Shielded1 uH10 %25 mA600 mOhms - 55 C+ 125 C35125 MHzStandard1.6 mm0.8 mm0.8 mm Ferrite AIML - 0603Reel , Cut Tape
MHQ0402PSA1N1BT000


RF Inductors - SMD 01005, 1.1nH +-0.1nH S-HQ SMD RF IND
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TDK 70328
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AUD 0.0248
Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded1.1 nH0.1 nH500 mA150 mOhms-- 55 C+ 125 C1020 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQW15AN36NG80D


RF Inductors - SMD 36 NH 2%
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Murata 70245
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AUD 0.104
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Wirewound0402 (1005 METRIC)Unshielded36 nH2 %540 mA309 mOhms-- 55 C+ 125 C303.8 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQP03TNR12J02D


RF Inductors - SMD 120 NH 5%
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Murata 69713
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AUD 0.0231
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Thin Film0201 (0603 METRIC)Unshielded120 nH5 %80 mA12 Ohms - 55 C+ 125 C8800 MHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
PE-0402CL2N0STT


RF Inductors - SMD 0402 2nH 300mA DCR=200mOhms RF
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Pulse 69126
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AUD 0.0264
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded2 nH0.3 nH300 mA200 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
B82422A1223K100


RF Inductors - SMD 22uH 140mA 10% 1210 SMD, AEC-Q200
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TDK 68443
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AUD 0.1947
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Wirewound1210 (3225 METRIC)Unshielded22 uH10 %140 mA2.65 Ohms-- 55 C+ 145 C2716 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
CIGT252010EH1R0MNE


RF Inductors - SMD CIGT,Thin Film,1008,1.0uH,1.0?,7 embossed,-20 20%
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SAMSUNG 67549
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AUD 0.1383
Multiples of: 1

Thin Film Unshielded1 uH20 %4.1 A30 mOhms4.7 A- 40 C+ 125 C--Standard2 mm1.25 mm0.8 mm-  CIGTReel , Cut Tape
LQW18ANR10G00D


RF Inductors - SMD .1 UH 2%
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Murata 56279
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AUD 0.0433
Multiples of: 20

Wirewound0603 (1608 METRIC)Unshielded100 nH2 %220 mA680 mOhms-- 55 C+ 125 C341.8 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
LQP03TN2N9B02D


RF Inductors - SMD 2.9 NH +-.1NH
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Murata 55775
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AUD 0.0059
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded2.9 nH0.1 nH500 mA200 mOhms - 55 C+ 125 C149.5 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP03TN0N6B02D


RF Inductors - SMD .6 NH
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Murata 53447
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AUD 0.0055
Multiples of: 100

Thin Film0201 (0603 METRIC)Unshielded600 pH0.1 nH850 mA70 mOhms - 55 C+ 125 C1420 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
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