HM61-20221LFTR13

DC Resistance (DCR):	950 mOhm
Height - Seated (Max):	0.224" (5.70mm)
Size / Dimension:	0.335" L x 0.250" W (8.51mm x 6.35mm)
Supplier Device Package:	--
Package / Case:	Nonstandard
Mounting Type:	Surface Mount
Inductance Frequency - Test:	1kHz
Operating Temperature:	-40°C ~ 155°C
Ratings:	--
Frequency - Self Resonant:	5.2MHz
Q @ Freq:	--
Series:	HM61
Shielding:	Unshielded
Current - Saturation:	--
Current Rating:	570mA
Tolerance:	±10%
Inductance:	220µH
Material - Core:	--
Type:	Wirewound
Part Status:	Discontinued at Digi-Key
Packaging:	Tape & Reel (TR)

Due to market price fluctuations, if you need to purchase or consult the price. You can contact us or emial to us:   sales@allicdata.com

The use of fixed inductors in electrical circuits is growing in popularity, and among the most popular fixed inductor models is the HM61-20221LFTR13. This versatile and reliable model is suitable for a variety of purposes and can be used for both AC and DC electrical systems ranging from regulated power supplies, electronic automotive control systems, and high-frequency RF circuits.The construction of the HM61-20221LFTR13 varies significantly from other inductor models. Its core is made of highly ferromagnetic material which gives it the capability to produce large inductance with a relatively small size. Its low profile design gives it a great deal of stability and the low level of frequency response combined with its large inductance rating makes it an ideal choice for high current applications.The basic working principle of the HM61-20221LFTR13 is based on Faraday\'s law of induction. According to this law, when a change in magnetic flux passes through a coil due to a changing magnetic field, an electric current is induced in the coil which is proportional to the rate of change in the magnetic field. The HM61-20221LFTR13 uses this principle to convert electrical energy into an oscillating magnetic field, which in turn induces an electric current in the coil.The magnetic field generated by the HM61-20221LFTR13 is relatively constant over a wide frequency range, and this makes it suitable for both AC and DC circuits. In AC circuits, the HM61-20221LFTR13 can be used to create a low-impedance path for the flow of electric current. This helps to regulate the current and reduce the risk of over voltage or under voltage conditions.In DC circuits, the HM61-20221LFTR13 can be used to minimize parasitic reactance. This results in a lower EMI emission which can be beneficial in applications such as RF circuits where electromagnetic interference is a major concern. In addition, the low inductance of the HM61-20221LFTR13 reduces the inductive losses associated with the load, allowing for a higher efficiency in the circuit.The HM61-20221LFTR13 is highly reliable and is a cost-effective solution for many applications. It offers a good balance between price and performance and is suitable for a variety of applications including regulated power supplies, electronic automotive control systems, and high-frequency RF circuits. In summary, the HM61-20221LFTR13 can be classified as a fixed inductor. It utilizes Faraday\'s law of induction to generate an oscillating magnetic field, which induces an electric current in a coil. This current can be used to regulate the flow of electrical energy, reduce EMI emissions, and minimize inductive losses. The HM61-20221LFTR13 is a reliable and cost-effective solution for many applications and is suitable for AC and DC circuits.

The specific data is subject to PDF, and the above content is for reference

Part Number	Manufacturer	Price	Quantity	Description