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The article discusses the concept of energy storage in an inductor, explaining how inductors store energy in their magnetic fields rather than dissipating it as heat. It covers the mathematical formulation for calculating stored energy, the behavior of ideal and practical inductors, and provides an example calculation to illustrate the concept.
Thus, the power delivered to the inductor p = v *i is also zero, which means that the rate of energy storage is zero as well. Therefore, the energy is only stored inside the inductor before its current reaches its maximum steady-state value, Im. After the current becomes constant, the energy within the magnetic becomes constant as well.
Figure 1 Determining the energy stored by an inductor In resistance circuits where the current and voltage do not change with a change in time, the energy transferred from the source to the resistance is W = Pt = VIt. Although the voltage remains constant in the circuit of Figure 1 (a), the current steadily increases as time elapses.
Without the internal resistance, the inductor is lossless because it cannot produce heat or light from the available energy. Therefore, all the energy supplied by the source ends up being stored in the generated magnetic field – exactly how energy is stored in rubber bands when stretched.
Some common hazards related to the energy stored in inductors are as follows: When an inductive circuit is completed, the inductor begins storing energy in its magnetic fields. When the same circuit is broken, the energy in the magnetic field is quickly reconverted into electrical energy.
Another safety consideration is to verify the de-energized state of inductors. Any residual energy in inductors can cause sparks if the leads are abruptly disconnected. The exponential characteristics of a practical inductor differ from the linear behavior of ideal inductors; both store energy similarly–by building up their magnetic fields.
