Lenz Law

The Lenz Law

The Lenz Law is called after the German-American mathematician and electro-physiologist, August Lenz. Lenz's law, in electricity, states that an electrical current flowing in a magnetic field constantly moves at precisely the same way as the Bar magnet it originally started with. The first reference to this particular law is found in H.G. Maxwell's"Theorie of Electricity" at 18societies and Electricity, Volumes I & II. Although this legislation is referred to as a classic illustration of electromagnetic theory, it's not without controversy.

For example, G.W. Maxwell found that the magnetic field formed by means of a magnet towards a point opposite it always matched the induced field shaped by a similar Strong magnet towards a stage in the center of the induced field. But by comparing the positions of those two poles of the magnet and people of the point contrary to the magnet, Maxwell demonstrated that there was such a force that induced both poles of the magnet to proceed with another, but not the other way around.

This led him to conclude that an electric current flowing in a wire through a really thin insulated wire in a circuit does not experience a change in its own value for infinite time, thus ruling out the introduction of an induced current. Thus, by assuming that the changes in the value of the induced current due to the motion of a magnet towards a point in the induced area does not last for infinity days, we arrive in another significant result of this Lenz Law. In accordance with this legislation, there is a point on a circuit whose induced magnetic field is zero, and the shifting magnetic field due to the movement of a magnet towards such a point will induce the induced current to begin at this point and push it out into the other end. In effect, such a point is known as a zero turn stage.