Experimental report on energy storage and discharge process of inductor

What is energy stored in an inductor?

Energy Stored in an Inductor Key Takeaways Understanding the energy stored in an inductor is crucial for various electrical and electronic applications, including power supplies, transformers, and energy storage systems. Inductors play a vital role in regulating current flow, filtering signals, and managing energy transfer in circuits.

What happens when an inductor reaches a steady-state value?

When the current in a practical inductor reaches its steady-state value of Im = E/R, the magnetic field ceases to expand. The voltage across the inductance has dropped to zero, so the power p = vi is also zero. Thus, the energy stored by the inductor increases only while the current is building up to its steady-state value.

How does a Magnetic Inductor store energy?

Instead, the energy is stored in the magnetic field as the rising current forces the magnetic lines of force to expand against their tendency to become as short as possible—somewhat as a rubber band stores energy when it is stretched. Figure 1 Determining the energy stored by an inductor

What is the area under the power curve of a Magnetic Inductor?

Current must continue to flow to maintain the magnetic field. The area under the power curve in Figure 2 represents the energy stored by the inductance and is equal to the product of the average power and the elapsed time. The energy stored in the magnetic field of an inductor can be written as:

How does a Magnetic Inductor increase if a current is constant?

The voltage across the inductance has dropped to zero, so the power p = vi is also zero. Thus, the energy stored by the inductor increases only while the current is building up to its steady-state value. When the current remains constant, the energy stored in the magnetic field is also constant.

What happens if an ideal inductor is connected to a voltage source?

If we connect an ideal inductor to a voltage source having no internal resistance, the voltage across the inductance must remain equal to the applied voltage. Therefore, the current rises at a constant rate, as shown in Figure 1 (b). The source supplies electrical energy to the ideal inductor at the rate of p = Ei.