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
  
                         
ASCH001005056N8JCP


RF Inductors - SMD 1005 6.8nH AEC-Q200
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Pulse 63525
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AUD 0.0377
Multiples of: 1

 1 mm x 0.5 mm x 0.5 mmShielded6.8 nH5 %400 mA240 mOhms-- 55 C+ 125 C84.55 GHzStandard1 mm0.5 mm0.5 mm- AEC - Q200ASCHReel , Cut Tape
LQG15HS1N0B02D


RF Inductors - SMD 1.0 NH +-.1NH
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Murata 63514
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AUD 0.0413
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded1 nH0.1 nH1 A70 mOhms-- 55 C+ 125 C810 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
CIGT201610EH2R2MNE


RF Inductors - SMD CIGT,Thin Film,0806,2.2uH,1.0?,7 embossed,-20 20%
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Samsung 62365
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AUD 0.132
Multiples of: 1

Thin Film Shielded2.2 uH20 %2.5 A74 mOhms2.7 A- 40 C+ 125 C--Standard2 mm1.6 mm1 mm-Metal Composite CIGTReel , Cut Tape
LQP03HQ4N3H02D


RF Inductors - SMD 4.3 NH 3%
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Murata 58510
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AUD 0.0332
Multiples of: 20

Thin Film0201 (0603 METRIC)Unshielded4.3 nH3 %500 mA170 mOhms-- 55 C+ 125 C207 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
LQG15HN10NJ02D


RF Inductors - SMD 10 NH 5%
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Murata 58200
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AUD 0.0092
Multiples of: 10000

Multilayer0402 (1005 METRIC)Unshielded10 nH5 %500 mA290 mOhms - 55 C+ 125 C83.2 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQG15HZ39NJ02D


RF Inductors - SMD 39 NH .2%
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Murata 44051
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AUD 0.0379
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded39 nH5 %300 mA650 mOhms - 55 C+ 125 C81.2 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
KLZ1608MHR100WTD25


RF Inductors - SMD 10uH 2MHz 20% 1608 AEC-Q200
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TDK 34984
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AUD 0.1172
Multiples of: 1

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
LQP03TN15NH02D


RF Inductors - SMD 15 NH 3%
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Murata 27063
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AUD 0.0109
Multiples of: 100

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
LQW15AN2N7G8ZD


RF Inductors - SMD 2.7 NH 2%
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Murata 17760
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AUD 0.1056
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded2.7 nH2 %1.5 A47 mOhms-- 55 C+ 125 C2814 GHzStandard1 mm0.6 mm0.5 mm-FerriteAEC - Q200LQWReel , Cut Tape
LQG15HZ8N2H02D


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 9700
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AUD 0.0324
Multiples of: 20

Multilayer0402 (1005 METRIC)Unshielded8.2 nH3 %550 mA240 mOhms - 55 C+ 125 C83.7 GHzStandard1 mm0.5 mm0.5 mm-AirAEC - Q200LQGReel , Cut Tape
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