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
  
                         
B82496C3109A


RF Inductors - SMD 1.0nH mA ohms
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TDK 58121
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AUD 0.2079
Multiples of: 1

Wirewound0603 (1608 METRIC)Unshielded1 nH0.3 nH1.8 A20 mOhms-- 55 C+ 150 C716 GHzStandard1.6 mm0.8 mm0.8 mm-CeramicAEC - Q200SIMID - CReel , Cut Tape
LQP03TN2N7B02D


RF Inductors - SMD 2.7 NH
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Murata 57618
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AUD 0.0174
Multiples of: 50

Thin Film0201 (0603 METRIC)Unshielded2.7 nH0.1 nH500 mA200 mOhms - 55 C+ 125 C1410 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
LQP02HQ0N5W02L


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 57103
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AUD 0.0957
Multiples of: 1

Thin Film01005 (0402 METRIC)Unshielded500 pH0.05 nH1 A40 mOhms - 55 C+ 125 C1420 GHzStandard0.4 mm0.2 mm0.3 mm-Ferrite LQPReel , 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
LQP03TQ1N8C02D


RF Inductors - SMD 1.8nH 650mA 0201 (0603 metric) SUGGESTED ALT LQP03HQ1N8C02D
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Murata 56577
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AUD 0.0294
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded1.8 nH0.2 nH650 mA100 mOhms-- 55 C+ 125 C1715 GHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
MLG1005S1N0BT000


RF Inductors - SMD IND 0402 1.0nH StdQ SMD RF IND
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TDK 55998
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AUD 0.0087
Multiples of: 10

Multilayer0402 (1005 METRIC)Unshielded1 nH0.1 nH1 A100 mOhms-- 55 C+ 125 C713.8 GHzStandard1 mm0.5 mm0.5 mm-Ceramic MLGReel , Cut Tape
LQW15AN4N7B00D


RF Inductors - SMD 4.7 NH +-.1NH
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Murata 55910
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AUD 0.081
Multiples of: 10

Wirewound0402 (1005 METRIC)Unshielded4.7 nH0.1 nH750 mA70 mOhms-- 55 C+ 125 C258 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQP03TNR15J02D


RF Inductors - SMD 150 NH 3%
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Murata 55581
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AUD 0.0281
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded150 nH5 %80 mA9 Ohms - 55 C+ 125 C5650 MHzStandard0.6 mm0.3 mm0.3 mm-Ferrite LQPReel , Cut Tape
BSCH0010050556NJCS


RF Inductors - SMD Chilisin RF inductor Multilayer-STD
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Pulse 55193
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AUD 0.0189
Multiples of: 1

 1 mm x 0.5 mm x 0.5 mmShielded56 nH5 % 1.3 Ohms150 mA- 55 C+ 125 C81.3 GHzStandard1 mm0.5 mm0.5 mm Ceramic BSCHReel , Cut Tape
LQW15AN3N0B80D


RF Inductors - SMD 3 NH +-.1 NH
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Murata 55143
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AUD 0.1122
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded3 nH0.1 nH1.35 A63 mOhms-- 55 C+ 125 C2012.5 GHzStandard1 mm0.6 mm0.6 mm-  LQWReel , Cut Tape
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