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
  
                         
LQG15HZ10NJ02D


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 19812
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AUD 0.0422
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Multilayer0402 (1005 METRIC)Unshielded10 nH5 %500 mA260 mOhms-- 55 C+ 125 C83.4 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQP03HQ0N9B02D


RF Inductors - SMD
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Murata 19789
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AUD 0.0901
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Thin Film0201 (0603 METRIC)Unshielded900 pH0.1 nH1.1 A40 mOhms-- 55 C+ 125 C2018 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
LQP03HQ3N7B02D


RF Inductors - SMD
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Murata 19733
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AUD 0.0862
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Thin Film0201 (0603 METRIC)Unshielded3.7 nH0.1 nH500 mA170 mOhms-- 55 C+ 125 C207 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
LQG15WH2N7C02D


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 19711
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AUD 0.0848
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Multilayer0402 (1005 METRIC)Unshielded2.7 nH0.2 nH900 mA70 mOhms-- 55 C+ 125 C236.5 GHzStandard1 mm0.6 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
LQP03HQ1N9B02D


RF Inductors - SMD 1.9 NH +/-0.1NH
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Murata 19692
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AUD 0.0835
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Thin Film0201 (0603 METRIC)Unshielded1.9 nH0.1 nH600 mA120 mOhms-- 55 C+ 125 C2010 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
CWF1610-2R2K


RF Inductors - SMD Ind,1.6x1x1mm,2.2uH+/-10%,0.58A,non-shd
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Bourns 19587
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AUD 0.0891
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Wirewound0603 (1610 METRIC)Semi - Shielded2.2 uH10 %580 mA -- 40 C+ 125 C--Standard1.6 mm1 mm1 mm-Ferrite CWF1610Reel , Cut Tape
MHQ0603P33NJT000


RF Inductors - SMD IND 0201 33nH S-HQ SMD RF IND
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TDK 19493
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AUD 0.043
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Multilayer0201 (0603 METRIC)Unshielded33 nH5 %160 mA2.8 Ohms-- 55 C+ 125 C142.5 GHzStandard0.65 mm0.35 mm0.35 mm-Ceramic MHQ - PReel , Cut Tape
AIMC-0402-5N6S-T


RF Inductors - SMD FIXED IND 5.6NH 300MA 300 MOHM
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ABRACON 19457
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AUD 0.0256
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Multilayer Ceramic Chip Inductor0402 (1005 METRIC)Shielded5.6 nH0.3 nH300 mA230 mOhms - 55 C+ 125 C94 GHzStandard1 mm0.5 mm0.5 mm Ceramic AIMC - 0402Reel , Cut Tape
MLG1005S22NJTD25


RF Inductors - SMD IND 0402 22nH StdQ AEC Q200 RF IND
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TDK 19446
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AUD 0.0245
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Multilayer0402 (1005 METRIC)Unshielded22 nH5 %350 mA700 mOhms-- 55 C+ 125 C82.2 GHzStandard1 mm0.5 mm0.5 mm-CeramicAEC - Q200MLGReel , Cut Tape
LQG15HN12NJ02D


RF Inductors - SMD 12 NH 5%
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Murata 16684
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AUD 0.008
Multiples of: 100

Multilayer0402 (1005 METRIC)Unshielded12 nH5 %400 mA400 mOhms-- 55 C+ 125 C82.8 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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