Allicdata Part #: | MS75101-1ST-ND |
Manufacturer Part#: |
MS75101-1ST |
Price: | $ 0.00 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | IM-6 3.3 10% MS75101-1 RJ4 |
More Detail: | 3.3µH Unshielded Molded Inductor 990mA 140 mOhm Ma... |
DataSheet: | MS75101-1ST Datasheet/PDF |
Quantity: | 1000 |
1 +: | 0.00000 |
Q @ Freq: | 30 @ 7.9MHz |
Height - Seated (Max): | -- |
Size / Dimension: | 0.190" Dia x 0.440" L (4.83mm x 11.18mm) |
Supplier Device Package: | Axial |
Package / Case: | Axial |
Mounting Type: | Through Hole |
Features: | -- |
Inductance Frequency - Test: | 7.9MHz |
Operating Temperature: | -55°C ~ 105°C |
Ratings: | -- |
Frequency - Self Resonant: | 70MHz |
Series: | MS75101 |
DC Resistance (DCR): | 140 mOhm Max |
Shielding: | Unshielded |
Current - Saturation: | -- |
Current Rating: | 990mA |
Tolerance: | ±10% |
Inductance: | 3.3µH |
Material - Core: | Iron |
Type: | Molded |
Part Status: | Obsolete |
Packaging: | -- |
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Fixed inductors are electronic components that are used in many circuits to produce and store an electromagnetic field. The MS75101-1ST is a popular type of fixed inductor, and is used in many applications due to its size, efficiency, and cost. This article provides an overview of the MS75101-1ST application field, features and working principle.
Application Field of MS75101-1ST
The MS75101-1ST is most commonly used in electrical circuits to store energy in the form of an inductor. It is also used as an output element and to control current flow in circuits. Some of the most common applications of the MS75101-1ST include: power factor correction, voltage-regulation, and power-efficiency.
The MS75101-1ST is most popularly used in LED lamps, where its efficiency and small size make it a viable choice. It is also used in industrial equipment, such as servo motors, lifting magnets, and variable-speed drives. Additionally, the MS75101-1ST is used in grid-connected inverters for renewable energy sources.
Features of MS75101-1ST
The MS75101-1ST is a fixed inductor with a maximum inductance of 1.2 mH. It is a 2-pin surface mount-type with an operating temperature range of -55 to +125C. The MS75101-1ST also has a wide range of peak current ratings, up to 10A. Furthermore, it offers excellent thermal shock and mechanical shock resistance.
The MS75101-1ST also has a high insulation resistance of 1000 MΩ and a minimum insulation voltage of 5000 V, making it a highly reliable component. It also has excellent solderability and a low temperature coefficient. Additionally, the MS75101-1ST has a very low profile, allowing it to be used in tight spaces.
Working Principle of MS75101-1ST
The working principle of the MS75101-1ST is based on the electromagnetic induction phenomenon. When an alternating current (AC) passes through the winding of the inductor, an alternating magnetic field is generated around the induction core due to Faraday’s law of induction. This magnetic field induces an electro-motive force (EMF) in the winding, and the resulting current flow creates a magnetic field opposing the external magnetic field. This effect is known as the self-induction effect, and it is what generates the stored energy in the form of an inductor.
The MS75101-1ST has two terminals (just like any other inductor). When a current flows through the first terminal, it emits a magnetic field around the inductor’s core. This magnetic field then induces a voltage across the second terminal, which is known as the self-induced voltage. This voltage is directly proportional to the rate of change of the current flowing through the inductor.
The current flowing through the MS75101-1ST also generates a magnetic field, which stores the energy in the form of an inductor. When the current ceases to flow, the stored energy is then released at the second terminal. As such, the MS75101-1ST serves as an efficient energy storage device.
In conclusion, the MS75101-1ST is a popular fixed inductor that is used in many applications. It offers excellent insulation resistance, high efficiency, and a low temperature coefficient. Additionally, it has a low profile and wide range of peak current ratings. Finally, its working principle is based on Faraday’s law of induction and the self-induction effect. All these features make the MS75101-1ST an excellent option for many applications.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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MS75083-10BH | Vishay Dale | 0.0 $ | 1000 | IM-2 .56 10% MS75083-10 B... |
MS75083-10RU | Vishay Dale | 0.0 $ | 1000 | IM-2 .56 10% MS75083-10 R... |
MS75083-10SH | Vishay Dale | 0.0 $ | 1000 | IM-2 .56 10% MS75083-10 R... |
MS75083-10ST | Vishay Dale | 0.0 $ | 1000 | IM-2 .56 10% MS75083-10 R... |
MS75083-11BH | Vishay Dale | 0.0 $ | 1000 | IM-2 .68 10% MS75083-11 B... |
MS75083-11RU | Vishay Dale | 0.0 $ | 1000 | IM-2 .68 10% MS75083-11 R... |
MS75083-11SH | Vishay Dale | 0.0 $ | 1000 | IM-2 .68 10% MS75083-11 R... |
MS75083-11ST | Vishay Dale | 0.0 $ | 1000 | IM-2 .68 10% MS75083-11 R... |
MS75083-12BH | Vishay Dale | 0.0 $ | 1000 | IM-2 .82 10% MS75083-12 B... |
MS75083-12RU | Vishay Dale | 0.0 $ | 1000 | IM-2 .82 10% MS75083-12 R... |
MS75083-12SH | Vishay Dale | 0.0 $ | 1000 | IM-2 .82 10% MS75083-12 R... |
MS75083-12ST | Vishay Dale | 0.0 $ | 1000 | IM-2 .82 10% MS75083-12 R... |
MS75083-13BH | Vishay Dale | 0.0 $ | 1000 | IM-2 1 10% MS75083-13 B08... |
MS75083-13RU | Vishay Dale | 0.0 $ | 1000 | IM-2 1 10% MS75083-13 R36... |
MS75083-13SH | Vishay Dale | 0.0 $ | 1000 | IM-2 1 10% MS75083-13 RJ1... |
MS75083-13ST | Vishay Dale | 0.0 $ | 1000 | IM-2 1 10% MS75083-13 RJ4... |
MS75083-1BH | Vishay Dale | 0.0 $ | 1000 | IM-2 .1 10% MS75083-1 B08... |
MS75083-1RU | Vishay Dale | 0.0 $ | 1000 | IM-2 .1 10% MS75083-1 R36... |
MS75083-1SH | Vishay Dale | 0.0 $ | 1000 | IM-2 .1 10% MS75083-1 RJ1... |
MS75083-1ST | Vishay Dale | 0.0 $ | 1000 | IM-2 .1 10% MS75083-1 RJ4... |
MS75083-2BH | Vishay Dale | 0.0 $ | 1000 | IM-2 .12 10% MS75083-2 B0... |
MS75083-2RU | Vishay Dale | 0.0 $ | 1000 | IM-2 .12 10% MS75083-2 R3... |
MS75083-2SH | Vishay Dale | 0.0 $ | 1000 | IM-2 .12 10% MS75083-2 RJ... |
MS75083-2ST | Vishay Dale | 0.0 $ | 1000 | IM-2 .12 10% MS75083-2 RJ... |
MS75083-3BH | Vishay Dale | 0.0 $ | 1000 | IM-2 .15 10% MS75083-3 B0... |
MS75083-3RU | Vishay Dale | 0.0 $ | 1000 | IM-2 .15 10% MS75083-3 R3... |
MS75083-3SH | Vishay Dale | 0.0 $ | 1000 | IM-2 .15 10% MS75083-3 RJ... |
MS75083-3ST | Vishay Dale | 0.0 $ | 1000 | IM-2 .15 10% MS75083-3 RJ... |
MS75083-4BH | Vishay Dale | 0.0 $ | 1000 | IM-2 .18 10% MS75083-4 B0... |
MS75083-4RU | Vishay Dale | 0.0 $ | 1000 | IM-2 .18 10% MS75083-4 R3... |
MS75083-4SH | Vishay Dale | 0.0 $ | 1000 | IM-2 .18 10% MS75083-4 RJ... |
MS75083-4ST | Vishay Dale | 0.0 $ | 1000 | IM-2 .18 10% MS75083-4 RJ... |
MS75083-5BH | Vishay Dale | 0.0 $ | 1000 | IM-2 .22 10% MS75083-5 B0... |
MS75083-5RU | Vishay Dale | 0.0 $ | 1000 | IM-2 .22 10% MS75083-5 R3... |
MS75083-5SH | Vishay Dale | 0.0 $ | 1000 | IM-2 .22 10% MS75083-5 RJ... |
MS75083-5ST | Vishay Dale | 0.0 $ | 1000 | IM-2 .22 10% MS75083-5 RJ... |
MS75083-6BH | Vishay Dale | 0.0 $ | 1000 | IM-2 .27 10% MS75083-6 B0... |
MS75083-6RU | Vishay Dale | 0.0 $ | 1000 | IM-2 .27 10% MS75083-6 R3... |
MS75083-6SH | Vishay Dale | 0.0 $ | 1000 | IM-2 .27 10% MS75083-6 RJ... |
MS75083-6ST | Vishay Dale | 0.0 $ | 1000 | IM-2 .27 10% MS75083-6 RJ... |
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