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
  
                         
BSCH0010050510NJCS


RF Inductors - SMD 1005 10nH
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Pulse 124593
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AUD 0.0198
Multiples of: 1

 1 mm x 0.5 mm x 0.5 mmShielded10 nH5 % 260 mOhms300 mA- 55 C+ 125 C83.9 GHzStandard1 mm0.5 mm0.5 mm-Ceramic BSCHReel , Cut Tape
BSCH000603038N2J00


RF Inductors - SMD 0603 8.2nH
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Pulse 123844
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AUD 0.0173
Multiples of: 1

 0.6 mm x 0.3 mm x 0.3 mmShielded8.2 nH5 % 450 mOhms230 mA- 55 C+ 125 C43.4 GHzStandard0.6 mm0.3 mm0.3 mm-Ceramic BSCHReel , Cut Tape
LQG15HS1N3S02D


RF Inductors - SMD 1.3 NH +-.3NH
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Murata 120668
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AUD 0.019
Multiples of: 50

Multilayer0402 (1005 METRIC)Unshielded1.3 nH0.3 nH1 A70 mOhms-- 55 C+ 125 C86 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
MHQ0603P0N8CT000


RF Inductors - SMD IND 0201 0.8nH S-HQ SMD RF IND
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TDK 120236
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AUD 0.0462
Multiples of: 1

Multilayer0201 (0603 METRIC)Unshielded800 pH0.2 nH1 A70 mOhms-- 55 C+ 125 C-20 GHzStandard0.65 mm0.35 mm0.35 mm Ceramic MHQ - PReel , Cut Tape
CIGT201208EHR47MNE


RF Inductors - SMD CIGT,Thin Film,0805,0.47uH,0.8?,7 embossed,-20 20%
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SAMSUNG 119895
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AUD 0.132
Multiples of: 1

Thin Film Unshielded470 nH20 %4.1 A35 mOhms4.3 A- 40 C+ 125 C--Standard2 mm1.25 mm0.8 mm-  CIGTReel , Cut Tape
LQW15AN33NJ80D


RF Inductors - SMD 33 NH 5%
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Murata 118898
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AUD 0.0941
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded33 nH5 %620 mA336 mOhms-- 55 C+ 125 C303.6 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
LQW15AN47NJ00D


RF Inductors - SMD 47 NH 5%
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Murata 118058
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AUD 0.0502
Multiples of: 10

Wirewound0402 (1005 METRIC)Unshielded47 nH5 %210 mA1.08 Ohms-- 55 C+ 125 C252.9 GHzStandard1 mm0.5 mm0.5 mm-  LQWReel , Cut Tape
LQW18AN18NG00D


RF Inductors - SMD 18 NH 2%
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Murata 114906
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AUD 0.0456
Multiples of: 20

Wirewound0603 (1608 METRIC)Unshielded18 nH2 %550 mA160 mOhms-- 55 C+ 125 C405.5 GHzStandard1.6 mm0.8 mm0.8 mm-  LQWReel , Cut Tape
PE-0402CL470JTT


RF Inductors - SMD 0402 47nH 200mA DCR=11000mOhms RF
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Pulse 113349
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AUD 0.0315
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded47 nH5 %200 mA1.1 Ohms-- 55 C+ 125 C81 GHzStandard1 mm0.5 mm0.5 mm-Ceramic PE - 0402CLReel , Cut Tape
CIGT201610UM1R0MNE


RF Inductors - SMD CIGT,Thin Film,0806,1.0uH,1.0?,7 embossed,-20 20%
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Samsung 113112
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AUD 0.104
Multiples of: 1

Thin Film  1 uH20 %              CIGTReel , Cut Tape
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