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
  
                         
PE-0402CL8N2JTT


RF Inductors - SMD 0402 8.2nH 300mA DCR=400mOhms RF
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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.

Pulse 90411
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AUD 0.0315
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded8.2 nH5 %300 mA400 mOhms - 55 C+ 125 C83.6 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
MHQ0402PSA0N8BT000


RF Inductors - SMD 01005, 0.8nH +-0.1nH S-HQ SMD RF IND
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TDK 86603
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AUD 0.0264
Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded800 pH0.1 nH600 mA150 mOhms-- 55 C+ 125 C-20 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
CIGT201610LH2R2MNE


RF Inductors - SMD CIGT,Thin Film,0806,2.2uH,1.0?,7 embossed,-20 20%
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Samsung 85329
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AUD 0.1232
Multiples of: 1

Thin Film Shielded2.2 uH20 %1.8 A139 mOhms2 A- 40 C+ 125 C--Standard2 mm1.6 mm1 mm-Metal Composite CIGTReel , Cut Tape
PE-0402CL3N9STT


RF Inductors - SMD 0402 3.9nH 300mA DCR=200mOhms RF
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Pulse 84448
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AUD 0.0315
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded3.9 nH0.3 nH300 mA200 mOhms-- 55 C+ 125 C84 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
MHQ1005P3N0BT000


RF Inductors - SMD IND 0402 3.0nH S-HQ SMD RF IND
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TDK 83090
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AUD 0.0427
Multiples of: 20

Multilayer0402 (1005 METRIC)Unshielded3 nH0.1 nH900 mA80 mOhms-- 55 C+ 125 C239.4 GHzStandard1 mm0.5 mm0.6 mm-Ceramic MHQ - PReel , Cut Tape
LQW18AN6N8G80D


RF Inductors - SMD 6.8 NH 2%
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Murata 82948
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AUD 0.099
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded6.8 nH2 %1.9 A40 mOhms-- 55 C+ 125 C406.65 GHzStandard1.65 mm0.99 mm0.9 mm-  LQWReel , Cut Tape
LQP03TN15NH02D


RF Inductors - SMD 15 NH 3%
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Murata 82595
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AUD 0.0154
Multiples of: 50

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
LQP03TN1N8B02D


RF Inductors - SMD 1.8 NH +-.1NH
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Murata 82401
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AUD 0.0146
Multiples of: 50

Thin Film0201 (0603 METRIC)Unshielded1.8 nH0.1 nH600 mA150 mOhms - 55 C+ 125 C1415 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQG15HS1N0S02D


RF Inductors - SMD 1.0 NH +-.3NH
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Murata 81601
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AUD 0.0264
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded1 nH0.3 nH1 A70 mOhms-- 55 C+ 125 C810 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQG15HS3N3B02D


RF Inductors - SMD 3.3 NH +/-0.1NH
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Murata 77852
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AUD 0.0259
Multiples of: 20

Multilayer0402 (1005 METRIC)Unshielded3.3 nH0.1 nH800 mA125 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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