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
  
                         
LQP03TN1N8B02D


RF Inductors - SMD 1.8 NH +-.1NH
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Murata 71101
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AUD 0.0074
Multiples of: 100

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
KLZ1608MHR100WTD25


RF Inductors - SMD 10uH 2MHz 20% 1608 AEC-Q200
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TDK 62080
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AUD 0.1207
Multiples of: 4000

Multilayer0603 (1608 METRIC)Shielded10 uH20 %250 mA1.05 Ohms90 mA- 55 C+ 150 C--Flexible (Soft)1.6 mm0.8 mm0.95 mm-FerriteAEC - Q200KLZ - HRReel , Cut Tape
LQP02HQ0N4W02L


RF Inductors - 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.

Murata 60304
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AUD 0.0983
Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded400 pH0.05 nH1 A30 mOhms-- 55 C+ 125 C1420 GHzStandard0.4 mm0.2 mm0.3 mm-  LQPReel , Cut Tape
LQW15AN3N9G80D


RF Inductors - SMD 3.9 NH 2%
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Murata 60208
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AUD 0.112
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded3.9 nH2 %1.95 A30 mOhms-- 55 C+ 125 C3510 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQG15HN10NJ02D


RF Inductors - SMD 10 NH 5%
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Murata 58200
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AUD 0.0096
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded10 nH5 %500 mA290 mOhms - 55 C+ 125 C83.2 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
CIGT201610LH1R0MNE


RF Inductors - SMD CIGT,Thin Film,0806,1.0uH,1.0?,7 embossed,-20 20%
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SAMSUNG 58025
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AUD 0.0936
Multiples of: 1

Thin Film  1 uH20 %              CIGTReel , Cut Tape
BSCH0016080822NJ00


RF Inductors - SMD 22nH RDC=0.40Ohms 500mA
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Pulse 57101
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AUD 0.0443
Multiples of: 1

 1.6 mm x 0.8 mm x 0.8 mmShielded22 nH5 % 400 mOhms500 mA- 55 C+ 125 C122 GHzStandard1.6 mm0.8 mm0.8 mm-Ceramic BSCHReel , Cut Tape
CIGT252010EH2R2MNE


RF Inductors - SMD CIGT,Thin Film,1008,2.2uH,1.0?,7 embossed,-20 20%
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Samsung 57002
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AUD 0.1737
Multiples of: 1

Thin Film Shielded2.2 uH20 %2.61 A77 mOhms2.5 A- 40 C+ 125 C--Standard2.5 mm2 mm1 mm-Metal Composite CIGTReel , Cut Tape
LQG15HN1N8B02D


RF Inductors - 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.

Murata 56226
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AUD 0.0465
Multiples of: 1

Multilayer Unshielded1.8 nH30 %900 mA80 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
B82422-A1103-K100


RF Inductors - SMD 10uH 180mA 10% 1210 SMD, AEC-Q200
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TDK 56199
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AUD 0.2552
Multiples of: 1

Wirewound1210 (3225 METRIC)Unshielded10 uH10 %180 mA1.6 Ohms-- 55 C+ 145 C2725 MHzStandard3.2 mm2.5 mm2 mm-FerriteAEC - Q200B82422AReel , Cut Tape
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