Siemens Fixed Inductors 19

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Part	Manufacturer	Inductor Type	Inductor Application	No. of Terminals	Shielded	Surface Mount	Minimum Quality Factor (at L-nom)	Terminal Finish	Self Resonance Frequency	Terminal Placement	DC Resistance	No. of Functions	Core Material	Test Frequency	Special Feature	Tolerance	JESD-609 Code	Shape or Size Description	Terminal Shape	Nominal Inductance (L)	Maximum Rated Current
B82422-A1103-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	27	Tin	25 MHz	Dual Ended	1.6 Ω	1	Ferrite	1 MHz	Q measured at 2.52 MHz	10 %	e3	Rectangular Package	J Bend	10 μH	180 mA
B82422-A1102-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	20	Tin	320 MHz	Dual Ended	340 mΩ	1	Ferrite	1 MHz	Q measured at 7.96 MHz	10 %	e3	Rectangular Package	J Bend	1 μH	380 mA
B82422-A1104-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	27	Tin	7 MHz	Dual Ended	11.5 Ω	1	Ferrite	100 kHz	Q measured at 2.52 MHz	10 %	e3	Rectangular Package	J Bend	100 μH	65 mA
B82422-A1682-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	27	Tin	55 MHz	Dual Ended	2.8 Ω	1	Ferrite	1 MHz	Q measured at 7.96 MHz	10 %	e3	Rectangular Package	J Bend	6.8 μH	135 mA
B82422-A1333-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	27	Tin	13 MHz	Dual Ended	4.5 Ω	1	Ferrite	100 kHz	Q measured at 2.52 MHz	10 %	e3	Rectangular Package	J Bend	33 μH	105 mA
B82422-A1332-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	27	Tin	75 MHz	Dual Ended	1.2 Ω	1	Ferrite	1 MHz	Q measured at 7.96 MHz	10 %	e3	Rectangular Package	J Bend	3.3 μH	200 mA
B82422-A1392-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	27	Tin	70 MHz	Dual Ended	1.4 Ω	1	Ferrite	1 MHz	Q measured at 7.96 MHz	10 %	e3	Rectangular Package	J Bend	3.9 μH	190 mA
B82422-A1823-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	27	Tin	8 MHz	Dual Ended	10 Ω	1	Ferrite	100 kHz	Q measured at 2.52 MHz	10 %	e3	Rectangular Package	J Bend	82 μH	70 mA
B82422-A3471-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	22	Tin	480 MHz	Dual Ended	2.2 Ω	1	Ceramic	1 MHz	Q measured at 30 MHz	10 %	e3	Rectangular Package	J Bend	470 nH	150 mA
B82422-A3470-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	26	Tin	1350 MHz	Dual Ended	190 mΩ	1	Ceramic	10 MHz	Q measured at 50 MHz	10 %	e3	Rectangular Package	J Bend	47 nH	510 mA
B82422-A3120-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	25	Tin	2500 MHz	Dual Ended	100 mΩ	1	Ceramic	10 MHz	Q measured at 100 MHz	10 %	e3	Rectangular Package	J Bend	12 nH	700 mA
B82422-A1222-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	25	Tin	125 MHz	Dual Ended	750 mΩ	1	Ferrite	1 MHz	Q measured at 7.96 MHz	10 %	e3	Rectangular Package	J Bend	2.2 μH	270 mA
B82422-A1472-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	27	Tin	65 MHz	Dual Ended	2.2 Ω	1	Ferrite	1 MHz	Q measured at 7.96 MHz	10 %	e3	Rectangular Package	J Bend	4.7 μH	150 mA
B82422-A1473-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	27	Tin	11 MHz	Dual Ended	7 Ω	1	Ferrite	100 kHz	Q measured at 2.52 MHz	10 %	e3	Rectangular Package	J Bend	47 μH	85 mA
B82422-A1683-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	27	Tin	9 MHz	Dual Ended	7.7 Ω	1	Ferrite	100 kHz	Q measured at 2.52 MHz	10 %	e3	Rectangular Package	J Bend	68 μH	80 mA
B82422-A1822-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	27	Tin	50 MHz	Dual Ended	3 Ω	1	Ferrite	1 MHz	Q measured at 7.96 MHz	10 %	e3	Rectangular Package	J Bend	8.2 μH	130 mA
B82422-A3271-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	20	Tin	650 MHz	Dual Ended	900 mΩ	1	Ceramic	1 MHz	Q measured at 30 MHz	10 %	e3	Rectangular Package	J Bend	270 nH	235 mA
B82422-A3681-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	22	Tin	180 MHz	Dual Ended	2.4 Ω	1	Ceramic	1 MHz	Q measured at 30 MHz	10 %	e3	Rectangular Package	J Bend	680 nH	145 mA
B82422-A3121-K100	Siemens	General Purpose Inductor	RF Inductor	2	No	Yes	22	Tin	880 MHz	Dual Ended	320 mΩ	1	Ceramic	1 MHz	Q measured at 30 MHz	10 %	e3	Rectangular Package	J Bend	120 nH	400 mA

Fixed Inductors

Fixed inductors, also known as passive inductors, are electronic components that are designed to store energy in a magnetic field. These components are used in a wide range of electronic applications, including power supplies, filters, oscillators, and RF circuits.

Fixed inductors can be classified into several types based on their specific characteristics and applications. Some of the most common types of fixed inductors include:

1. Wire-wound inductors - These inductors consist of a wire coil wound around a core, typically made of a magnetic material such as iron or ferrite. Wire-wound inductors are commonly used in power supplies and filters.

2. Multilayer ceramic inductors - These inductors are made by stacking thin layers of ceramic material with metal electrodes. Multilayer ceramic inductors are commonly used in high-frequency applications due to their high Q factor and small size.

3. Ferrite bead inductors - These inductors consist of a cylindrical or toroidal ferrite bead that is threaded onto a wire or placed over a PCB trace. Ferrite bead inductors are commonly used in EMI suppression and RF filtering applications.

Fixed inductors are available in a wide range of inductance values, sizes, and power ratings. They are typically characterized by their inductance value, tolerance, and frequency response. Inductance is measured in henries (H) or millihenries (mH), and tolerance refers to the allowed deviation from the specified inductance value.