Allicdata Part #: | 587-5883-2-ND |
Manufacturer Part#: |
LBR2012T100M |
Price: | $ 0.00 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Taiyo Yuden |
Short Description: | FIXED IND 10UH 150MA 360 MOHM |
More Detail: | 10µH Unshielded Wirewound Inductor 150mA 360 mOhm ... |
DataSheet: | LBR2012T100M Datasheet/PDF |
Quantity: | 12000 |
Specifications
DC Resistance (DCR): | 360 mOhm |
Height - Seated (Max): | 0.057" (1.45mm) |
Size / Dimension: | 0.079" L x 0.049" W (2.00mm x 1.25mm) |
Supplier Device Package: | 0805 (2012 Metric) |
Package / Case: | 0805 (2012 Metric) |
Mounting Type: | Surface Mount |
Inductance Frequency - Test: | 2.52MHz |
Operating Temperature: | -25°C ~ 105°C |
Ratings: | -- |
Frequency - Self Resonant: | 32MHz |
Q @ Freq: | -- |
Series: | LB, R Type |
Shielding: | Unshielded |
Current - Saturation: | -- |
Current Rating: | 150mA |
Tolerance: | ±20% |
Inductance: | 10µH |
Material - Core: | -- |
Type: | Wirewound |
Part Status: | Active |
Packaging: | Tape & Reel (TR) |
Description
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Fixed Inductors
Fixed inductors are electrical components that are used in circuits to store energy in the form of a magnetic field. Specifically, a fixed inductor is an electronic component consisting of a coil of wire wrapped around a core material. When an electrical current passes through the coil, a magnetic field is created. This field acts as an energy storage device, allowing the inductor to maintain an electrical charge for a period of time after the current stops flowing.The LBR2012T100M is a class of inductor that is designed with a variety of applications in mind. This type of fixed inductor provides a wide range of current capabilities, allowing it to be used in a wide variety of systems. Its primary use is in DC-DC converters, providing an inductive buffer between various components. The LBR2012T100M also has applications in power factor correction (PFC) circuits, telecom systems, and various other electronics and industrial electronics.The LBR2012T100M operates on the principle of Faraday’s Law of induction. When an electrical current is applied to the inductor, a time-varying magnetic field is created. The changing magnetic field induces an electric field in the inductor which counteracts the applied current, thus creating a resistive force against the flow of electrons. This resistance, known as inductance, is measured in Henrys (symbolized as H).Due to the high inductance of the LBR2012T100M, it is important to consider the effects of a parasitic capacitance when designing circuits. The presence of a capacitance can cause an inductor to generate harmonic frequencies, reducing the efficiency of the overall system. To counteract this effect, the LBR2012T100M is designed with a high inductance-to-capacitance ratio, reducing the extent of the unwanted harmonics and providing a more effective inductor.In addition to providing high efficiency, the LBR2012T100M is also designed to provide low losses in case of short circuit currents. This is because the inductor is designed to have a very low cross sectional area. This reduces the amount of heat that is generated during operation and minimizes losses in case of a short circuit occurring.The LBR2012T100M is designed to handle a wide range of current ratings, allowing it to be used in a variety of applications. For example, the inductor can handle currents from 1.0A to 10A. This makes it ideal for use in DC-DC converters and power factor correction circuits, as well as in other high-current applications.The LBR2012T100M is a fixed inductor designed to provide a wide range of current capabilities and high power-handling capabilities. It is designed to minimize harmonic distortion, providing an efficient inductor for use in many different applications. With its high inductance-to-capacitance ratio, low losses in case of short circuit current, and wide range of current ratings, the LBR2012T100M is an ideal choice for many different projects.The specific data is subject to PDF, and the above content is for reference
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LBR2012T470KV | Taiyo Yuden | 0.06 $ | 1000 | FIXED IND 47UH 75MA 1.7 O... |
LBR2012T220KV | Taiyo Yuden | 0.06 $ | 1000 | FIXED IND 22UH 100MA 1 OH... |
LBR2518T1R0M | Taiyo Yuden | -- | 2000 | FIXED IND 1UH 960MA 45 MO... |
LBR2518T101K | Taiyo Yuden | -- | 2000 | FIXED IND 100UH 80MA 1.89... |
LBR2012T100KV | Taiyo Yuden | 0.06 $ | 3000 | FIXED IND 10UH 150MA 360 ... |
LBR2012T101KV | Taiyo Yuden | 0.06 $ | 3000 | FIXED IND 100UH 50MA 4 OH... |
LBR2012T1R0MV | Taiyo Yuden | 0.06 $ | 3000 | FIXED IND 1UH 400MA 70 MO... |
LBR2518T101KV | Taiyo Yuden | 0.08 $ | 6000 | FIXED IND 100UH 80MA 1.89... |
LBR2518T100KV | Taiyo Yuden | 0.08 $ | 2000 | FIXED IND 10UH 235MA 190 ... |
LBR2012T100K | Taiyo Yuden | -- | 108000 | FIXED IND 10UH 150MA 360 ... |
LBR2012T1R0M | Taiyo Yuden | -- | 45000 | FIXED IND 1UH 400MA 91 MO... |
LBR2518T100K | Taiyo Yuden | 0.04 $ | 12000 | FIXED IND 10UH 235MA 190 ... |
LBR2012T4R7M | Taiyo Yuden | -- | 45000 | FIXED IND 4.7UH 200MA 240... |
LBR2012T470K | Taiyo Yuden | 0.04 $ | 1000 | FIXED IND 47UH 75MA 1.7 O... |
LBR2012T2R2M | Taiyo Yuden | 0.02 $ | 21000 | FIXED IND 2.2UH 260MA 130... |
LBR2012T470M | Taiyo Yuden | -- | 1000 | FIXED IND 47UH 75MA 1.7 O... |
LBR2518T220K | Taiyo Yuden | 0.04 $ | 1000 | FIXED IND 22UH 175MA 440 ... |
LBR2518T2R2M | Taiyo Yuden | 0.04 $ | 1000 | FIXED IND 2.2UH 480MA 70 ... |
LBR2012T2R2MV | Taiyo Yuden | 0.06 $ | 3000 | FIXED IND 2.2UH 260MA 130... |
LBR2518T220KV | Taiyo Yuden | 0.08 $ | 2000 | FIXED IND 22UH 175MA 440 ... |
LBR2518T2R2MV | Taiyo Yuden | 0.08 $ | 2000 | FIXED IND 2.2UH 480MA 70 ... |
LBR2518T470KV | Taiyo Yuden | 0.08 $ | 2000 | FIXED IND 47UH 120MA 840 ... |
LBR2518T4R7MV | Taiyo Yuden | 0.08 $ | 2000 | FIXED IND 4.7UH 345MA 100... |
LBR2012T101K | Taiyo Yuden | -- | 75000 | FIXED IND 100UH 50MA 4 OH... |
LBR2012T220K | Taiyo Yuden | 0.02 $ | 9000 | FIXED IND 22UH 100MA 1 OH... |
LBR2012T100M | Taiyo Yuden | -- | 12000 | FIXED IND 10UH 150MA 360 ... |
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