Allicdata Part #: | 399-9562-2-ND |
Manufacturer Part#: |
L0603B1R0MPWFT |
Price: | $ 0.10 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | KEMET |
Short Description: | FIXED IND 1UH 620MA 190 MOHM SMD |
More Detail: | 1µH Unshielded Wirewound Inductor 620mA 190 mOhm 0... |
DataSheet: | L0603B1R0MPWFT Datasheet/PDF |
Quantity: | 1000 |
3000 +: | $ 0.08921 |
6000 +: | $ 0.08397 |
15000 +: | $ 0.08135 |
30000 +: | $ 0.07872 |
75000 +: | $ 0.07610 |
DC Resistance (DCR): | 190 mOhm |
Height - Seated (Max): | 0.028" (0.71mm) |
Size / Dimension: | 0.063" L x 0.032" W (1.60mm x 0.81mm) |
Supplier Device Package: | 0603 (1608 Metric) |
Package / Case: | 0603 (1608 Metric) |
Mounting Type: | Surface Mount |
Inductance Frequency - Test: | 7.96MHz |
Operating Temperature: | -40°C ~ 105°C |
Ratings: | -- |
Frequency - Self Resonant: | 100MHz |
Q @ Freq: | -- |
Series: | L-PWF |
Shielding: | Unshielded |
Current - Saturation: | -- |
Current Rating: | 620mA |
Tolerance: | ±20% |
Inductance: | 1µH |
Material - Core: | Ferrite |
Type: | Wirewound |
Part Status: | Active |
Packaging: | Tape & Reel (TR) |
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Fixed inductors refer to a kind of electronic components that can store energy in a magnetic field. LO603B1R0MPWFT is a typical example of a fixed inductor, which is mostly designed and produced by Würth Elektronik. The simple circuits and wide range of inductance value makes LO603B1R0MPWFT suitable for many applications.
In terms of application fields, LO603B1R0MPWFT is mostly used in low-voltage, low-power electronic circuits, such as power supplies, DC/DC converters, charging circuits, drive circuits, signal filters and switching mode power supplies – SMPS. Besides, LO603B1R0MPWFT is also suitable for applications with high disruption requirements or for conditions requiring frequency reduction.
To understand the working principle of LO603B1R0MPWFT, we need to have a brief overview of the properties of inductance. Inductance is a physical phenomenon arising from the magnetic field generated by the flow of electric current through a material or structure. The magnetic fields generated by the flow of charge carriers around the coil of the inductor oppose the change in current, and a voltage is induced across the inductor. This voltage is the quantity that we call inductance. The inductance depends on the construction of the inductor, the shape of the coil, the intensity of the magnetic fields, the material of the coil, and the distance between the coil and the magnetic field.
In terms of construction, LO603B1R0MPWFT consists of a ferrite core and a thick layer of enameled copper wire. The core is made of a ferrite material which provides a strong magnetic field to concentrate the magnetic flux between the inductor and the environment. The enameled wire is a high-resilience material that makes sure the inductance does not deteriorate over time. The construction of the LO603B1R0MPWFT ensures a high saturation current, low heat build-up and a wide temperature range of use.
When current passes through the LO603B1R0MPWFT, a magnetic field is created around it and an inductance is induced. This inductance will oppose the current and force it to take a different path, depending on the strength of the inductance. The amount of voltage induced across the inductor is determined by the strength of the magnetic field, the size of the coil and the distance between the environment and the inductor. The LO603B1R0MPWFT is designed to have an optimum inductance, enabling it to handle high current and voltage.
In conclusion, LO603B1R0MPWFT is an example of a fixed inductor, designed for the applications in low-voltage, low-power electronic circuits, power supplies, DC/DC converters, charging circuits, drive circuits, signal filters and switching mode power supplies – SMPS. It has a ferrite core and thick layer of enameled wire, which provide high saturation current, low heat build-up and a wide temperature range of use. When current passes through the LO603B1R0MPWFT, a magnetic field is created around it and an inductance is induced. The amount of voltage induced across the inductor is determined by the strength of the magnetic field, the size of the coil and the distance between the environment and the inductor.
The specific data is subject to PDF, and the above content is for reference
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