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
  
                         
MHQ0402PSA3N3CT000


RF Inductors - SMD 01005, 3.3nH +-0.2nH S-HQ SMD RF IND
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TDK 16754
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AUD 0.0525
Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded3.3 nH0.2 nH250 mA650 mOhms-- 55 C+ 125 C109.46 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQG15HS8N2H02D


RF Inductors - SMD 8.2 NH 3%
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Murata 16753
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AUD 0.033
Multiples of: 1

Multilayer0402 (1005 METRIC)Unshielded8.2 nH3 %550 mA240 mOhms - 55 C+ 125 C83.7 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
LQW15AN7N1G80D


RF Inductors - SMD
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Murata 16693
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AUD 0.1072
Multiples of: 1

Wirewound0402 (1005 METRIC)Unshielded7.1 nH2 %1.42 A69 mOhms-- 55 C+ 125 C328.5 GHzStandard1 mm0.6 mm0.5 mm-  LQWReel , Cut Tape
MHQ0402PSA1N2BT000


RF Inductors - SMD 01005, 1.2nH +-0.1nH S-HQ SMD RF IND
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TDK 16692
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AUD 0.0255
Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded1.2 nH0.1 nH500 mA200 mOhms-- 55 C+ 125 C1016.72 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQP03HQ2N2C02D


600mA 2.2nH 120mO 0201 Inductors (SMD) ROHS
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Murata 16684
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AUD 0.0676
Multiples of: 1

Thin Film0201 (0603 METRIC)Unshielded2.2 nH0.2 nH600 mA120 mOhms-- 55 C+ 125 C209 GHzStandard0.6 mm0.3 mm0.4 mm-Ferrite LQPReel , Cut Tape
WCLA3225V1-221-R


RF Inductors - SMD Chip IND 202uH 0.115A SMT 2 Pad
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Eaton 16645
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AUD 0.286
Multiples of: 1

Wirewound1210 (3225 METRIC)Shielded220 uH10 %115 mA8.23 Ohms - 55 C+ 125 C104 MHz 3.6 mm2.8 mm2.4 mm Ferrite WCLAReel , Cut Tape
MHQ0402PSA3N9BT000


RF Inductors - SMD 01005, 3.9nH +-0.1nH S-HQ SMD RF IND
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TDK 16639
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AUD 0.0289
Multiples of: 1

Multilayer01005 (0402 METRIC)Unshielded3.9 nH0.1 nH200 mA750 mOhms-- 55 C+ 125 C108.91 GHzStandard0.4 mm0.2 mm0.2 mm-Ceramic MHQ - PSAReel , Cut Tape
LQP03TN3N0BZ2D


RF Inductors - SMD
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Murata 16481
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AUD 0.034
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Thin Film0201 (0603 METRIC)Unshielded3 nH0.1 nH450 mA250 mOhms - 55 C+ 125 C149.5 GHzStandard0.6 mm0.3 mm0.3 mm-FerriteAEC - Q200LQPReel , Cut Tape
CWF1610-150K


RF Inductors - SMD Ind,1.6x1x1mm,15uH+/-10%,0.24A,non-shd
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Bourns 12827
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AUD 0.1353
Multiples of: 1

Wirewound0603 (1610 METRIC)Semi - Shielded15 uH10 %240 mA -- 40 C+ 125 C--Standard1.6 mm1 mm1 mm-Ferrite CWF1610Reel , Cut Tape
LQG15HS18NH02D


RF Inductors - SMD 4.7 NH .2%
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Murata 9370
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AUD 0.0201
Multiples of: 20

Multilayer0402 (1005 METRIC)Unshielded18 nH3 %400 mA360 mOhms - 55 C+ 125 C82.2 GHzStandard1 mm0.5 mm0.5 mm-Air LQGReel , Cut Tape
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